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	<updated>2026-07-13T00:26:34Z</updated>
	<subtitle>User contributions</subtitle>
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	<entry>
		<id>https://tetrationforum.org/hyperops_wiki/index.php?title=File:Fps9_stb.png&amp;diff=223</id>
		<title>File:Fps9 stb.png</title>
		<link rel="alternate" type="text/html" href="https://tetrationforum.org/hyperops_wiki/index.php?title=File:Fps9_stb.png&amp;diff=223"/>
		<updated>2022-07-21T20:07:36Z</updated>

		<summary type="html">&lt;p&gt;Bo198214: Shows the fixed points of b^z for b moving along the Shell-Thron boundary&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Shows the fixed points of b^z for b moving along the Shell-Thron boundary&lt;/div&gt;</summary>
		<author><name>Bo198214</name></author>
	</entry>
	<entry>
		<id>https://tetrationforum.org/hyperops_wiki/index.php?title=Shell-Thron_region&amp;diff=203</id>
		<title>Shell-Thron region</title>
		<link rel="alternate" type="text/html" href="https://tetrationforum.org/hyperops_wiki/index.php?title=Shell-Thron_region&amp;diff=203"/>
		<updated>2019-07-16T19:09:38Z</updated>

		<summary type="html">&lt;p&gt;Bo198214: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;The Shell-Thron region is the region of complex numbers $b$ where the limit of the infinite exponential tower&lt;br /&gt;
$$\lambda=\lim_{n\to\infty} \exp_b^{\circ n}(1)$$&lt;br /&gt;
exists; to be explicit we mean the main branch of the power: $\exp_b(z):=b^z:=\exp(\log(b)z)$.&lt;br /&gt;
&lt;br /&gt;
If this limit $\lambda$ exists then must $b^\lambda=\lambda$, i.e. $\lambda$ must be a fixpoint of $f(z)=b^z$, or&lt;br /&gt;
$$\lambda=\frac{W(-\log(b))}{-\log(b)}$$&lt;br /&gt;
&lt;br /&gt;
By a result of Barrow the limit $\lambda$ exists exactly for all $b$ where $|\log(\lambda)|\le 1$. &lt;br /&gt;
&lt;br /&gt;
The boundary of the Thron-Shell region, i.e. all bases $b$ where $|\log(\lambda)|=1$, is given by all $b$ where $|\exp_b&amp;#039;(\lambda)|=1$ (i.e. lambda is a parabolic fixpoint of $\exp_b$) due to the following rearrangements:&lt;br /&gt;
$$\begin{align*}&lt;br /&gt;
1=|\exp_b&amp;#039;(\lambda)|=|\log(b)\exp_b(\lambda)|=|\log(b)\lambda|=|\log(b^\lambda)|=|\log(\lambda)|&lt;br /&gt;
\end{align*}$$&lt;br /&gt;
&lt;br /&gt;
These rearrangements are not proper derivations, but hints only, as with complex bases one always has to worry about landing in the right branch.&lt;br /&gt;
&lt;br /&gt;
Following from this the boundary can be given as a curve $\phi\mapsto \exp(e^{i\phi-e^{i\phi}}),\phi\in[0,2\pi)$.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;hr&amp;gt;&lt;br /&gt;
The following picture of the upper part of the Shell-Thron region was made by [[User:Andydude|Andrew]].       &lt;br /&gt;
&lt;br /&gt;
[[File:Shell-region.png]]     &lt;br /&gt;
&lt;br /&gt;
&amp;lt;hr&amp;gt;  &lt;br /&gt;
&lt;br /&gt;
This picture gives a combined view of the locus of the fixpoints, their logs (being on the unit-circle) and the corresponding complex bases: (the symbol $\lambda$ is replaced by the letter $t$ )     &lt;br /&gt;
[[File:ShellThron_utb.png|600px]]&lt;br /&gt;
&lt;br /&gt;
== Relevant posts on the Tetrationforum ==&lt;br /&gt;
&lt;br /&gt;
*  [http://math.eretrandre.org/tetrationforum/showthread.php?tid=263&amp;amp;pid=3011#pid3011 Question about infinite tetrate]       &lt;br /&gt;
&lt;br /&gt;
*  [http://math.eretrandre.org/tetrationforum/showthread.php?tid=120&amp;amp;pid=1377#pid1377 Infinite tetration of the imaginary unit]&lt;/div&gt;</summary>
		<author><name>Bo198214</name></author>
	</entry>
	<entry>
		<id>https://tetrationforum.org/hyperops_wiki/index.php?title=Shell-Thron_region&amp;diff=202</id>
		<title>Shell-Thron region</title>
		<link rel="alternate" type="text/html" href="https://tetrationforum.org/hyperops_wiki/index.php?title=Shell-Thron_region&amp;diff=202"/>
		<updated>2019-07-16T19:08:44Z</updated>

		<summary type="html">&lt;p&gt;Bo198214: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;The Shell-Thron region is the region of complex numbers $b$ where the limit of the infinite exponential tower&lt;br /&gt;
$$\lambda=\lim_{n\to\infty} \exp_b^{\circ n}(1)$$&lt;br /&gt;
exists; to be explicit we mean the main branch of the power: $\exp_b(z):=b^z:=\exp(\log(b)z)$.&lt;br /&gt;
&lt;br /&gt;
If this limit $\lambda$ exists then must $b^\lambda=\lambda$, i.e. $\lambda$ must be a fixpoint of $f(z)=b^z$, or&lt;br /&gt;
$$\lambda=\frac{W(-\log(b))}{-\log(b)}$$&lt;br /&gt;
&lt;br /&gt;
By a result of Barrow the limit $\lambda$ exists exactly for all $b$ where $|\log(\lambda)|\le 1$. &lt;br /&gt;
&lt;br /&gt;
The boundary of the Thron-Shell region, i.e. all bases $b$ where $|\log(\lambda)|=1$, is given by all $b$ where $|\exp_b&amp;#039;(\lambda)|=1$ (i.e. lambda is a parabolic fixpoint of $\exp_b$) due to the following rearrangements:&lt;br /&gt;
$$\begin{align*}&lt;br /&gt;
1=|\exp_b&amp;#039;(\lambda)|=|\log(b)\exp_b(\lambda)|=|\log(b)\lambda|=|\log(b^\lambda)|=|\log(\lambda)|&lt;br /&gt;
\end{align*}$$&lt;br /&gt;
&lt;br /&gt;
These rearrangements are not proper derivations, but hints only, as with complex bases one always has to worry about landing in the right branch.&lt;br /&gt;
&lt;br /&gt;
Following from this the boundary can be given as a curve $\phi\mapsto \exp(e^{i\phi-e^{i\phi}}),\phi\in(0,2\pi)$.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;hr&amp;gt;&lt;br /&gt;
The following picture of the upper part of the Shell-Thron region was made by [[User:Andydude|Andrew]].       &lt;br /&gt;
&lt;br /&gt;
[[File:Shell-region.png]]     &lt;br /&gt;
&lt;br /&gt;
&amp;lt;hr&amp;gt;  &lt;br /&gt;
&lt;br /&gt;
This picture gives a combined view of the locus of the fixpoints, their logs (being on the unit-circle) and the corresponding complex bases: (the symbol $\lambda$ is replaced by the letter $t$ )     &lt;br /&gt;
[[File:ShellThron_utb.png|600px]]&lt;br /&gt;
&lt;br /&gt;
== Relevant posts on the Tetrationforum ==&lt;br /&gt;
&lt;br /&gt;
*  [http://math.eretrandre.org/tetrationforum/showthread.php?tid=263&amp;amp;pid=3011#pid3011 Question about infinite tetrate]       &lt;br /&gt;
&lt;br /&gt;
*  [http://math.eretrandre.org/tetrationforum/showthread.php?tid=120&amp;amp;pid=1377#pid1377 Infinite tetration of the imaginary unit]&lt;/div&gt;</summary>
		<author><name>Bo198214</name></author>
	</entry>
	<entry>
		<id>https://tetrationforum.org/hyperops_wiki/index.php?title=Shell-Thron_region&amp;diff=201</id>
		<title>Shell-Thron region</title>
		<link rel="alternate" type="text/html" href="https://tetrationforum.org/hyperops_wiki/index.php?title=Shell-Thron_region&amp;diff=201"/>
		<updated>2019-07-16T19:08:08Z</updated>

		<summary type="html">&lt;p&gt;Bo198214: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;The Shell-Thron region is the region of complex numbers $b$ where the limit of the infinite exponential tower&lt;br /&gt;
$$\lambda=\lim_{n\to\infty} \exp_b^{\circ n}(1)$$&lt;br /&gt;
exists; to be explicit we mean the main branch of the power: $\exp_b(z):=b^z:=\exp(\log(b)z)$.&lt;br /&gt;
&lt;br /&gt;
If this limit $\lambda$ exists then must $b^\lambda=\lambda$, i.e. $\lambda$ must be a fixpoint of $f(z)=b^z$, or&lt;br /&gt;
$$\lambda=\frac{W(-\log(b))}{-\log(b)}$$&lt;br /&gt;
&lt;br /&gt;
By a result of Barrow the limit $\lambda$ exists exactly for all $b$ where $|\log(\lambda)|\le 1$. &lt;br /&gt;
&lt;br /&gt;
The boundary of the Thron-Shell region, i.e. all bases $b$ where $|\log(\lambda)|=1$, is given by all $b$ where $|\exp_b&amp;#039;(\lambda)|=1$ (i.e. lambda is a parabolic fixpoint of $\exp_b$) due to the following rearrangements:&lt;br /&gt;
$$\begin{align*}&lt;br /&gt;
1=|\exp_b&amp;#039;(\lambda)|=|\log(b)\exp_b(\lambda)|=|\log(b)\lambda|=|\log(b^\lambda)|=|\log(\lambda)|&lt;br /&gt;
\end{align*}$$&lt;br /&gt;
&lt;br /&gt;
These rearrangements are not proper derivations, but hints only, as with complex bases one always has to worry about landing in the right branch.&lt;br /&gt;
&lt;br /&gt;
Following from this the boundary can be given as a curve $\phi\mapsto exp(e^{i\phi-e^{i\phi}}),\phi\in(0,2\pi)$.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;hr&amp;gt;&lt;br /&gt;
The following picture of the upper part of the Shell-Thron region was made by [[User:Andydude|Andrew]].       &lt;br /&gt;
&lt;br /&gt;
[[File:Shell-region.png]]     &lt;br /&gt;
&lt;br /&gt;
&amp;lt;hr&amp;gt;  &lt;br /&gt;
&lt;br /&gt;
This picture gives a combined view of the locus of the fixpoints, their logs (being on the unit-circle) and the corresponding complex bases: (the symbol $\lambda$ is replaced by the letter $t$ )     &lt;br /&gt;
[[File:ShellThron_utb.png|600px]]&lt;br /&gt;
&lt;br /&gt;
== Relevant posts on the Tetrationforum ==&lt;br /&gt;
&lt;br /&gt;
*  [http://math.eretrandre.org/tetrationforum/showthread.php?tid=263&amp;amp;pid=3011#pid3011 Question about infinite tetrate]       &lt;br /&gt;
&lt;br /&gt;
*  [http://math.eretrandre.org/tetrationforum/showthread.php?tid=120&amp;amp;pid=1377#pid1377 Infinite tetration of the imaginary unit]&lt;/div&gt;</summary>
		<author><name>Bo198214</name></author>
	</entry>
	<entry>
		<id>https://tetrationforum.org/hyperops_wiki/index.php?title=Shell-Thron_region&amp;diff=200</id>
		<title>Shell-Thron region</title>
		<link rel="alternate" type="text/html" href="https://tetrationforum.org/hyperops_wiki/index.php?title=Shell-Thron_region&amp;diff=200"/>
		<updated>2019-07-16T18:41:59Z</updated>

		<summary type="html">&lt;p&gt;Bo198214: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;The Shell-Thron region is the region of complex numbers $b$ where the limit of the infinite exponential tower&lt;br /&gt;
$$\lambda=\lim_{n\to\infty} \exp_b^{\circ n}(1)$$&lt;br /&gt;
exists; to be explicit we mean the main branch of the power: $\exp_b(z):=b^z:=\exp(\log(b)z)$.&lt;br /&gt;
&lt;br /&gt;
If this limit $\lambda$ exists then must $b^\lambda=\lambda$, i.e. $\lambda$ must be a fixpoint of $f(z)=b^z$, or&lt;br /&gt;
$$\lambda=\frac{W(-\log(b))}{-\log(b)}$$&lt;br /&gt;
&lt;br /&gt;
By a result of Barrow the limit $\lambda$ exists exactly for all $b$ where $|\log(\lambda)|\le 1$. &lt;br /&gt;
&lt;br /&gt;
The boundary of the Thron-Shell region, i.e. all bases $b$ where $|\log(\lambda)|=1$, is given by all $b$ where $|\exp_b&amp;#039;(\lambda)|=1$ (i.e. lambda is a parabolic fixpoint of $\exp_b$) due to the following rearrangements:&lt;br /&gt;
$$\begin{align*}&lt;br /&gt;
1=|\exp_b&amp;#039;(\lambda)|=|\log(b)\exp_b(\lambda)|=|\log(b)\lambda|=|\log(b^\lambda)|=|\log(\lambda)|&lt;br /&gt;
\end{align*}$$&lt;br /&gt;
&lt;br /&gt;
These rearrangements are not proper derivations, but hints only, as with complex bases one always has to worry about landing in the right branch.&lt;br /&gt;
&lt;br /&gt;
The boundary can also be given by the formula $|-W(-\log(b))|=1$.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;hr&amp;gt;&lt;br /&gt;
The following picture of the upper part of the Shell-Thron region was made by [[User:Andydude|Andrew]].       &lt;br /&gt;
&lt;br /&gt;
[[File:Shell-region.png]]     &lt;br /&gt;
&lt;br /&gt;
&amp;lt;hr&amp;gt;  &lt;br /&gt;
&lt;br /&gt;
This picture gives a combined view of the locus of the fixpoints, their logs (being on the unit-circle) and the corresponding complex bases: (the symbol $\lambda$ is replaced by the letter $t$ )     &lt;br /&gt;
[[File:ShellThron_utb.png|600px]]&lt;br /&gt;
&lt;br /&gt;
== Relevant posts on the Tetrationforum ==&lt;br /&gt;
&lt;br /&gt;
*  [http://math.eretrandre.org/tetrationforum/showthread.php?tid=263&amp;amp;pid=3011#pid3011 Question about infinite tetrate]       &lt;br /&gt;
&lt;br /&gt;
*  [http://math.eretrandre.org/tetrationforum/showthread.php?tid=120&amp;amp;pid=1377#pid1377 Infinite tetration of the imaginary unit]&lt;/div&gt;</summary>
		<author><name>Bo198214</name></author>
	</entry>
	<entry>
		<id>https://tetrationforum.org/hyperops_wiki/index.php?title=Shishikura_perturbed_Fatou_coordinates&amp;diff=199</id>
		<title>Shishikura perturbed Fatou coordinates</title>
		<link rel="alternate" type="text/html" href="https://tetrationforum.org/hyperops_wiki/index.php?title=Shishikura_perturbed_Fatou_coordinates&amp;diff=199"/>
		<updated>2019-07-16T08:42:42Z</updated>

		<summary type="html">&lt;p&gt;Bo198214: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Shishikura writes&amp;lt;ref name=&amp;quot;Shishikura2000&amp;quot;&amp;gt;Shishikura, M. (2000). Bifurcation of parabolic fixed points. In Lei, Tan, The Mandelbrot set, theme and variations. Cambridge: Cambridge University Press. Lond. Math. Soc. Lect. Note Ser. 274, 325-363 (2000)&amp;lt;/ref&amp;gt; the following&lt;br /&gt;
&lt;br /&gt;
== $\mathcal{F}_0$ ==&lt;br /&gt;
&amp;amp;#91;p. 327&amp;amp;#93;&lt;br /&gt;
 &lt;br /&gt;
If $f_0&amp;#039;&amp;#039;(0)\neq 0$ by another coordinate change we may assume that $f_0&amp;#039;&amp;#039;(0)=1$, so define&lt;br /&gt;
$$ \mathcal{F}_0 = \{ f_0 \colon f_0 \quad\text{is defined and analytic in a neighborhood of 0}\quad f_0(0)=0, f_0&amp;#039;(0)=1, f_0&amp;#039;&amp;#039;(0)=1\}$$&lt;br /&gt;
&lt;br /&gt;
== Neighborhood of $f$ in the compact-open topology with domain of definition ==&lt;br /&gt;
&amp;amp;#91; p. 332 &amp;amp;#93;&lt;br /&gt;
&lt;br /&gt;
In what follows a map $f$ is always associated with its domain of definition $D(f)$. That is two maps are considered as distinct if they have distinct domains, even if the one is an extension of the other. A neighborhood of an analytic map $f\colon D(f)\to\overline{\C}$ is a set containing&lt;br /&gt;
$$\{ g \colon g \quad\text{is analytic},\quad D(g)\supset K, \sup_{z\in K} d(f(z)-g(z))&amp;lt;\eps \} $$&lt;br /&gt;
where $K$ is a compact set in $D(f)$, $\eps&amp;gt;0$ and $d(.,.)$ is the spherical metric.&lt;br /&gt;
A sequence $(f_n)$ converges to $f$ in this topology if and only if for any compact set $K\subset D(f)$ there exists $n_0$ such that $K\subset D(f_n)$ for all $n\ge n_0$ and $f_n|_K\to f|_K$ uniformly on $K$ as $n\to\infty$. The system of these neighborhoods define the &amp;quot;compact-open topology together with the domain of defintion&amp;quot;, which is unfortunately not Hausdorff, since an extension of $f$ is contained in any neighborhood of $f$.&lt;br /&gt;
&lt;br /&gt;
For $b_1,b_2\in\C$ with $\Re(b_1)&amp;lt;\Re(b_2)$ define &lt;br /&gt;
$$Q(b_1,b_2)=\{z\in\C\colon \Re(z-b_1)&amp;gt;-|\Im(z-b_1)|, \Re(z-b_2)&amp;gt;|\Im(z-b_2)|\}$$&lt;br /&gt;
If $b_1=-\infty$ (resp. $b_2=\infty$) then the corresponding condition should be removed.&lt;br /&gt;
&lt;br /&gt;
== Proposition 2.5.2 ==&lt;br /&gt;
&amp;amp;#91;p. 333&amp;amp;#93;&lt;br /&gt;
&lt;br /&gt;
Let $f$ be a holomorphic function defined on $Q=Q(b_1,b_2)$ with $\Re(b_2)&amp;gt;\Re(b_1)+2$ (here $b_1$ or $b_2$ may be $-\infty$ or $\infty$). Suppose &lt;br /&gt;
$$|F(z)-(z+1)|&amp;lt;\frac{1}{4},\quad |F&amp;#039;(z)-(z+1)|&amp;lt;\frac{1}{4}\quad \text{for all}\quad z\in Q.$$&lt;br /&gt;
&lt;br /&gt;
Then&lt;br /&gt;
# $F$ is univalent &amp;amp;#91;means injective&amp;amp;#93; on $Q$.&lt;br /&gt;
# Let $z_0\in Q$ be a point such that $\Re(b_1)&amp;lt;\Re(z_0)&amp;lt;\Re(b_2)-\frac{5}{4}$. Denote by $S$ the closed region (a strip) bounded by the two curves $\ell=\{z_0+i y\colon y\in\R\}$ and $F(\ell)$. Then for any $z\in Q$ there exist a unique $n\in \Z$ such that $F^n(z)$ is defined and belongs to $S-F(\ell)$.&lt;br /&gt;
# There exists an univalent function $\Phi\colon Q\to \C$ satisfying $$\Phi(F(z))=\Phi(z)+1$$ whenever both sides are defined. Moreover $\Phi$ is unique up to an addition of a constant.&lt;br /&gt;
# Fix a point $z_0\in Q$. If we normalize $\Phi$ by $\Phi(z_0)=0$ then the correspondence $F\mapsto \Phi$ is continuous with respect to the compact-open topology.&lt;br /&gt;
&lt;br /&gt;
== $\mathcal{F}$, $\mathcal{F}_1$ and $\alpha(f)$ ==&lt;br /&gt;
&amp;amp;#91;p. 339&amp;amp;#93;&lt;br /&gt;
&lt;br /&gt;
$$ \mathcal{F} = \{ f \colon f \quad\text{is defined and analytic in a neighborhood of 0}\quad f(0)=0, f_0&amp;#039;(0)\neq 0\}$$&lt;br /&gt;
For $f\in \mathcal{F}$ we express the derivative &lt;br /&gt;
$$f&amp;#039;(0)=\exp(2\pi i \alpha(f))$$&lt;br /&gt;
where $\alpha(f)\in\C$ and $-\frac{1}{2} &amp;lt; \Re(\alpha(f)) \le \frac{1}{2}$ our study is focussed on the maps in the following class&lt;br /&gt;
$$ \mathcal{F}_1 = \{ f\in \mathcal{F}\colon |\arg(\alpha(f))| &amp;lt; \frac{\pi}{4}\} $$&lt;br /&gt;
&lt;br /&gt;
=== Comments ===&lt;br /&gt;
&lt;br /&gt;
By the definition we have $$&lt;br /&gt;
\begin{align*}&lt;br /&gt;
\log(f&amp;#039;(0))&amp;amp;=2\pi i\alpha(f)=2\pi i re^{i\beta}=2\pi r e^{i(\beta+\frac{\pi}{2})}\\&lt;br /&gt;
\arg(\log(f&amp;#039;(0))&amp;amp;=\beta+\frac{\pi}{2}&lt;br /&gt;
\end{align*}$$&lt;br /&gt;
so the condition for $\mathcal{F}_1$ is&lt;br /&gt;
$|\arg(\log(f&amp;#039;(0)))-\frac{\pi}{2}|&amp;lt;\frac{\pi}{4}$ or&lt;br /&gt;
$$\frac{\pi}{4} &amp;lt; \arg(\log(f&amp;#039;(0)) &amp;lt; \frac{3\pi}{4}$$&lt;br /&gt;
&lt;br /&gt;
== $\sigma(f)$ ==&lt;br /&gt;
&amp;amp;#91;p. 340&amp;amp;#93;&lt;br /&gt;
&lt;br /&gt;
Let $\sigma(f)$ be the other fixpoint of $f$ (besides 0).&lt;br /&gt;
&lt;br /&gt;
...&lt;br /&gt;
&lt;br /&gt;
$$\sigma(f) = 2\pi i \alpha(f)(1+o(1)), \quad\text{as}\quad f\to f_0$$&lt;br /&gt;
&lt;br /&gt;
=== Comments ===&lt;br /&gt;
&lt;br /&gt;
By the comment before, we can say that $\sigma(f)$ lies roughly in the sector of angle $(\frac{\pi}{4},\frac{3\pi}{4})$ above the tip 0.&lt;br /&gt;
&lt;br /&gt;
== Proposition 3.2.2 ==&lt;br /&gt;
[p. 340]&lt;br /&gt;
&lt;br /&gt;
Let $f_0\in\mathcal{F}_0$. There exists a neighborhood $\mathcal{N}_0$ of $f_0$ (in the sense of the topology defined in 2.5.1) such that if $f\in\mathcal{N}_0\cap \mathcal{F}_1$, then there exist closed Jordan domains $S_{-,f}$, $S_{+,f}$ and analytic functions $\Phi_{-,f}$, $\Phi_{+,f}$ satisfying the following:&lt;br /&gt;
&lt;br /&gt;
# $S_{\pm,f}$ is bounded by an arc $\ell_{\pm}$ and its image $f(\ell_{\pm})$ such that $\ell_{\pm}$ joins two fixed points $\{0,\sigma(f)\}$, $\ell_{\pm}\cap f(\ell_{\pm}) = \{0,\sigma(f)\}$ and $S_{-,f}\cap S_{+,f} = \{0,\sigma(f)\}$; &lt;br /&gt;
# $\Phi_{\pm,f}$ is defined, analytic and injective in a neighborhood of $S&amp;#039;_{\pm,f} = S_{\pm,f}\setminus \{0,\sigma(f)\}$;&lt;br /&gt;
# if $z\in S&amp;#039;_{-,f}$ then there is an $n\ge 1$ such that $f^n(z)\in S&amp;#039;_{+,f}$ and for the smallest such $n$, \[ \Phi_{+,f}(f^n(z)) = \Phi_{-,f}(z) - \frac{1}{\alpha(f)} + n \]&lt;br /&gt;
# when $f\in\mathcal{F}_1$ tends to $f_0$, $S_{\pm,f}\to S_{\pm,0}\cup \{0\}$ in the Hausdorff metric, and $\Phi_{\pm,f}\to \Phi_{\pm,0}$ in the topology defined in 2.5.1.&lt;br /&gt;
&lt;br /&gt;
== Proposition 4.4.1 ==&lt;br /&gt;
&amp;amp;#91;p. 356&amp;amp;#93;&lt;br /&gt;
&lt;br /&gt;
Let $f_0\in\mathcal{F}_0$, there exists a neighborhood $\mathcal{N}_0$ of $f_0$ (in the previously described &amp;quot;compact-open topology with domain of definition&amp;quot;), such that if $f\in \mathcal{N}_0 \cap \mathcal{F}_1$, then there exist large $\xi_0, \eta_0&amp;gt;0$, and analytic maps $\ph_f\colon D(\ph_f)\to\overline{\C}$ and $\tilde{\mathcal{R}}_f\colon D(\tilde{\mathcal{R}}_f)\to \C$ satisfying the following:&lt;br /&gt;
# $D(\ph_f)$ contains the set $$ \mathcal{Q}_f = \{ w\in\C\colon |\arg(-w-\xi_0)| &amp;lt; \frac{2\pi}{3}, |\arg(w+\frac{1}{\alpha(f)}-\xi_0)|&amp;lt;\frac{2\pi}{3} \} $$ and $\ph_f(D(\ph_f)) \subseteq D(f)$; If $w, w+1\in D(\ph_f)$ then $$ \ph_f(w+1)=f(\ph_f(w)) $$ $\ph_f(w)\to 0$ when $w\in \mathcal{Q}_f$ and $\Im(w)\to\infty$; $\ph_f(w)\to\sigma(f)$ when $w\in\mathcal{Q}_f$ and $\Im(w)\to -\infty$.&lt;br /&gt;
# $D(\tilde{\mathcal{R}}_f)$ contains $\{ w\in\C\colon |\Im(w)| &amp;gt; \eta_0\}$ and is invariant under $T(w)=w+1$; if $w\in D(\tilde{\mathcal{R}}_f)$ then $$\tilde{\mathcal{R}}_f(w+1)=\tilde{\mathcal{R}}(w)+1;$$ $\tilde{\mathcal{R}}_f(w)-w$ tends to $-\frac{1}{\alpha(f)}$ when $\Im(w)\to\infty$; to a constant when $\Im(w)\to -\infty$.&lt;br /&gt;
# If $w\in D(\tilde{\mathcal{R}}_f)\cap D(\ph_f)$ and $w&amp;#039;=\tilde{\mathcal{R}}_f(w)+n\in D(\ph_f)$ for some $n\in\Z$ then $$f^n(\ph_f(w))=\ph_f(w&amp;#039;)\quad \text{for}\quad n\ge 0, \quad f^{-n}(\ph_f(w&amp;#039;))=\ph_f(w)\quad \text{for}\quad n&amp;lt;0$$ Moreover if $|\arg(w&amp;#039;+\frac{1}{2\alpha(f)}-\xi_0)|&amp;lt;\frac{2\pi}{3}$ then $n&amp;gt;0$.&lt;br /&gt;
# When $f\in\mathcal{F_1}$ and $f\to f_0$ $$\ph_f\to\ph_0\quad\text{and}\quad \tilde{\mathcal{R}}_f + \frac{1}{\alpha(f)} \to \tilde{\mathcal{E}}_{f_0}$$&lt;br /&gt;
&lt;br /&gt;
== Proposition A.1 ==&lt;br /&gt;
[p. 360]&lt;br /&gt;
&lt;br /&gt;
In the settings of Proposition 3.2.2 (resp. 2.5.2), assume in addtion that $f_s(z)$ (resp. $F_s(z)$) is a family of holomorphic maps for $s\in \Delta \cup \{0\} \subset \mathbb{C}^k$, with $\Delta\subset\mathbb{C}^k$ an open connected set containing 0 in the boundary, such that $f_s$ (resp. $F_s(z)$) is continuous for $s\in\Delta\cup \{0\}$ and analytic in $s\in\Delta$, then the Fatou coordinates $\Phi_{\pm,f_s}$ (resp. $\Phi_{F_s}$) depend analytically on $s$ for $s\in\Delta$.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;references/&amp;gt;&lt;/div&gt;</summary>
		<author><name>Bo198214</name></author>
	</entry>
	<entry>
		<id>https://tetrationforum.org/hyperops_wiki/index.php?title=Uniqueness_of_Tetration&amp;diff=195</id>
		<title>Uniqueness of Tetration</title>
		<link rel="alternate" type="text/html" href="https://tetrationforum.org/hyperops_wiki/index.php?title=Uniqueness_of_Tetration&amp;diff=195"/>
		<updated>2017-01-04T08:04:23Z</updated>

		<summary type="html">&lt;p&gt;Bo198214: work in progress&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&amp;#039;&amp;#039;&amp;#039;This is work in progress, dont rely on it!&amp;#039;&amp;#039;&amp;#039;&lt;br /&gt;
&lt;br /&gt;
== Proposition ==&lt;br /&gt;
For each $b&amp;gt;e^{1/e}$ there exists exactly one holomorphic function $\sigma_b$ on $D=\C\setminus\{x \le -2\}$ which is real for all $x&amp;gt;-2$ and satisfies for all $z\in D$:&lt;br /&gt;
$$\sigma_b(0)=1, \sigma_b(z+1)=b^{\sigma_b(z)}$$ and $$\sup_{t\to\infty}\left| \sigma_b({\rm i}t)\right| &amp;lt;\infty$$.&lt;br /&gt;
&lt;br /&gt;
==== Proof. ====&lt;br /&gt;
We know there exists already a solution $\tau_b$ which satisfies all conditions and its inverse $\alpha_b$ which is a whole function and satisifies $\alpha_b(b^z)=\alpha_b(z)+1$.&lt;br /&gt;
Then we know that &lt;br /&gt;
$$\sup_{t\to\infty}\alpha_b(\sigma_b({\rm i}t))&amp;lt;\infty$$&lt;br /&gt;
and the function $\delta(z)=\alpha_b(\sigma_b(z))-z$, holomorphic on $D$, is periodic with period 1:&lt;br /&gt;
$$\delta(z+1)=(\alpha_b(\sigma_b(z+1))-(z+1)=\alpha_b(\sigma_b(z))-z=\delta_b(z)$$&lt;br /&gt;
and is real for $z &amp;gt; -2$ (and can be continued to $\R$) and can so be developed into a real Fourier-Series ($A_k$,  $\phi_k$ in $\R$):&lt;br /&gt;
&lt;br /&gt;
$$\delta(t)=\sum_{k=0}^{\infty}A_{k}\cos\left(2\pi kt-\varphi_{k}\right)$$&lt;br /&gt;
&lt;br /&gt;
$$\delta(z)=\sum_{k=0}^{\infty}\frac{A_{k}}{2}\left(\exp\left(2\pi {\rm i}kz-{\rm i}\varphi_{k}\right)+\exp\left(-2\pi {\rm i}kz+{\rm i}\varphi_{k}\right)\right)$$&lt;br /&gt;
$$\delta(x+{\rm i}y)=\sum_{k=0}^{\infty}\frac{A_{k}}{2}\left(\exp\left({\rm i}(2\pi kx-\varphi_{k})-2\pi k y\right)+\exp\left({\rm i}(-2\pi kx+\varphi_{k})+2\pi k y\right)\right)&lt;br /&gt;
=\sum_{k=0}^{\infty}\frac{A_{k}}{2}\left(\cos(2\pi kx-\varphi_{k})\left(\exp\left(-2\pi k y\right)+\exp(2\pi ky)\right)+{\rm i}\sin(2\pi kx-\varphi_{k})\left(-\exp\left(2\pi k y\right)+\exp(-2\pi ky)\right)\right)$$&lt;br /&gt;
&lt;br /&gt;
$$\Im(\delta(x+{\rm i}y)+x+{\rm i}y)=y+\sum_{k=0}^{\infty}\frac{A_{k}}{2}\left(-\exp\left(2\pi k y\right)+\exp(-2\pi ky)\right)\sin(2\pi kx-\varphi_{k})$$&lt;br /&gt;
&lt;br /&gt;
$$&lt;br /&gt;
\alpha_b(\sigma_b({\rm i}t))=\delta({\rm i}t)+{\rm i}t={\rm i}t+\sum_{k=0}^{\infty}\frac{A_{k}}{2}\left(\exp\left(-2\pi kt -{\rm i}\varphi_{k}\right)+\exp\left(2\pi kt+{\rm i}\varphi_{k}\right)\right)&lt;br /&gt;
$$&lt;br /&gt;
&lt;br /&gt;
But this expression can only be bounded with respect to $t$ if $A_k=0$ for all $k\ge 1$. Hence $\delta$ is a constant $c$ and $\sigma_b(z)=\tau_b(z+c)$.&lt;/div&gt;</summary>
		<author><name>Bo198214</name></author>
	</entry>
	<entry>
		<id>https://tetrationforum.org/hyperops_wiki/index.php?title=Uniqueness_of_Tetration&amp;diff=194</id>
		<title>Uniqueness of Tetration</title>
		<link rel="alternate" type="text/html" href="https://tetrationforum.org/hyperops_wiki/index.php?title=Uniqueness_of_Tetration&amp;diff=194"/>
		<updated>2017-01-03T19:44:58Z</updated>

		<summary type="html">&lt;p&gt;Bo198214: /* Proposition */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;This is work in progress, dont rely on it!&lt;br /&gt;
&lt;br /&gt;
== Proposition ==&lt;br /&gt;
For each $b&amp;gt;e^{1/e}$ there exists exactly one holomorphic function $\sigma_b$ on $D=\C\setminus\{x \le -2\}$ which is real for all $x&amp;gt;-2$ and satisfies for all $z\in D$:&lt;br /&gt;
$$\sigma_b(0)=1, \sigma_b(z+1)=b^{\sigma_b(z)}$$ and $$\sup_{t\to\infty}\left| \sigma_b({\rm i}t)\right| &amp;lt;\infty$$.&lt;br /&gt;
&lt;br /&gt;
==== Proof. ====&lt;br /&gt;
We know there exists already a solution $\tau_b$ which satisfies all conditions and its inverse $\alpha_b$ which is a whole function and satisifies $\alpha_b(b^z)=\alpha_b(z)+1$.&lt;br /&gt;
Then we know that &lt;br /&gt;
$$\sup_{t\to\infty}\alpha_b(\sigma_b({\rm i}t))&amp;lt;\infty$$&lt;br /&gt;
and the function $\delta(z)=\alpha_b(\sigma_b(z))-z$, holomorphic on $D$, is periodic with period 1:&lt;br /&gt;
$$\delta(z+1)=(\alpha_b(\sigma_b(z+1))-(z+1)=\alpha_b(\sigma_b(z))-z=\delta_b(z)$$&lt;br /&gt;
and is real for $z &amp;gt; -2$ (and can be continued to $\R$) and can so be developed into a real Fourier-Series ($A_k$,  $\phi_k$ in $\R$):&lt;br /&gt;
&lt;br /&gt;
$$\delta(t)=\sum_{k=0}^{\infty}A_{k}\cos\left(2\pi kt-\varphi_{k}\right)$$&lt;br /&gt;
&lt;br /&gt;
$$\delta(z)=\sum_{k=0}^{\infty}\frac{A_{k}}{2}\left(\exp\left(2\pi {\rm i}kz-{\rm i}\varphi_{k}\right)+\exp\left(-2\pi {\rm i}kz+{\rm i}\varphi_{k}\right)\right)$$&lt;br /&gt;
$$\delta(x+{\rm i}y)=\sum_{k=0}^{\infty}\frac{A_{k}}{2}\left(\exp\left({\rm i}(2\pi kx-\varphi_{k})-2\pi k y\right)+\exp\left({\rm i}(-2\pi kx+\varphi_{k})+2\pi k y\right)\right)&lt;br /&gt;
=\sum_{k=0}^{\infty}\frac{A_{k}}{2}\left(\cos(2\pi kx-\varphi_{k})\left(\exp\left(-2\pi k y\right)+\exp(2\pi ky)\right)+{\rm i}\sin(2\pi kx-\varphi_{k})\left(-\exp\left(2\pi k y\right)+\exp(-2\pi ky)\right)\right)$$&lt;br /&gt;
&lt;br /&gt;
$$\Im(\delta(x+{\rm i}y)+x+{\rm i}y)=y+\sum_{k=0}^{\infty}\frac{A_{k}}{2}\left(-\exp\left(2\pi k y\right)+\exp(-2\pi ky)\right)\sin(2\pi kx-\varphi_{k})$$&lt;br /&gt;
&lt;br /&gt;
$$&lt;br /&gt;
\alpha_b(\sigma_b({\rm i}t))=\delta({\rm i}t)+{\rm i}t={\rm i}t+\sum_{k=0}^{\infty}\frac{A_{k}}{2}\left(\exp\left(-2\pi kt -{\rm i}\varphi_{k}\right)+\exp\left(2\pi kt+{\rm i}\varphi_{k}\right)\right)&lt;br /&gt;
$$&lt;br /&gt;
&lt;br /&gt;
But this expression can only be bounded with respect to $t$ if $A_k=0$ for all $k\ge 1$. Hence $\delta$ is a constant $c$ and $\sigma_b(z)=\tau_b(z+c)$.&lt;/div&gt;</summary>
		<author><name>Bo198214</name></author>
	</entry>
	<entry>
		<id>https://tetrationforum.org/hyperops_wiki/index.php?title=Uniqueness_of_Tetration&amp;diff=193</id>
		<title>Uniqueness of Tetration</title>
		<link rel="alternate" type="text/html" href="https://tetrationforum.org/hyperops_wiki/index.php?title=Uniqueness_of_Tetration&amp;diff=193"/>
		<updated>2017-01-03T19:44:25Z</updated>

		<summary type="html">&lt;p&gt;Bo198214: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Proposition ==&lt;br /&gt;
For each $b&amp;gt;e^{1/e}$ there exists exactly one holomorphic function $\sigma_b$ on $D=\C\setminus\{x \le -2\}$ which is real for all $x&amp;gt;-2$ and satisfies for all $z\in D$:&lt;br /&gt;
$$\sigma_b(0)=1, \sigma_b(z+1)=b^{\sigma_b(z)}$$ and $$\sup_{t\to\infty}\left| \sigma_b({\rm i}t)\right| &amp;lt;\infty$$.&lt;br /&gt;
&lt;br /&gt;
==== Proof. ====&lt;br /&gt;
We know there exists already a solution $\tau_b$ which satisfies all conditions and its inverse $\alpha_b$ which is a whole function and satisifies $\alpha_b(b^z)=\alpha_b(z)+1$.&lt;br /&gt;
Then we know that &lt;br /&gt;
$$\sup_{t\to\infty}\alpha_b(\sigma_b({\rm i}t))&amp;lt;\infty$$&lt;br /&gt;
and the function $\delta(z)=\alpha_b(\sigma_b(z))-z$, holomorphic on $D$, is periodic with period 1:&lt;br /&gt;
$$\delta(z+1)=(\alpha_b(\sigma_b(z+1))-(z+1)=\alpha_b(\sigma_b(z))-z=\delta_b(z)$$&lt;br /&gt;
and is real for $z &amp;gt; -2$ (and can be continued to $\R$) and can so be developed into a real Fourier-Series ($A_k$,  $\phi_k$ in $\R$):&lt;br /&gt;
&lt;br /&gt;
$$\delta(t)=\sum_{k=0}^{\infty}A_{k}\cos\left(2\pi kt-\varphi_{k}\right)$$&lt;br /&gt;
&lt;br /&gt;
$$\delta(z)=\sum_{k=0}^{\infty}\frac{A_{k}}{2}\left(\exp\left(2\pi {\rm i}kz-{\rm i}\varphi_{k}\right)+\exp\left(-2\pi {\rm i}kz+{\rm i}\varphi_{k}\right)\right)$$&lt;br /&gt;
$$\delta(x+{\rm i}y)=\sum_{k=0}^{\infty}\frac{A_{k}}{2}\left(\exp\left({\rm i}(2\pi kx-\varphi_{k})-2\pi k y\right)+\exp\left({\rm i}(-2\pi kx+\varphi_{k})+2\pi k y\right)\right)&lt;br /&gt;
=\sum_{k=0}^{\infty}\frac{A_{k}}{2}\left(\cos(2\pi kx-\varphi_{k})\left(\exp\left(-2\pi k y\right)+\exp(2\pi ky)\right)+{\rm i}\sin(2\pi kx-\varphi_{k})\left(-\exp\left(2\pi k y\right)+\exp(-2\pi ky)\right)\right)$$&lt;br /&gt;
&lt;br /&gt;
$$\Im(\delta(x+{\rm i}y)+x+{\rm i}y)=y+\sum_{k=0}^{\infty}\frac{A_{k}}{2}\left(-\exp\left(2\pi k y\right)+\exp(-2\pi ky)\right)\sin(2\pi kx-\varphi_{k})$$&lt;br /&gt;
&lt;br /&gt;
$$&lt;br /&gt;
\alpha_b(\sigma_b({\rm i}t))=\delta({\rm i}t)+{\rm i}t={\rm i}t+\sum_{k=0}^{\infty}\frac{A_{k}}{2}\left(\exp\left(-2\pi kt -{\rm i}\varphi_{k}\right)+\exp\left(2\pi kt+{\rm i}\varphi_{k}\right)\right)&lt;br /&gt;
$$&lt;br /&gt;
&lt;br /&gt;
But this expression can only be bounded with respect to $t$ if $A_k=0$ for all $k\ge 1$. Hence $\delta$ is a constant $c$ and $\sigma_b(z)=\tau_b(z+c)$.&lt;/div&gt;</summary>
		<author><name>Bo198214</name></author>
	</entry>
	<entry>
		<id>https://tetrationforum.org/hyperops_wiki/index.php?title=Uniqueness_of_Tetration&amp;diff=192</id>
		<title>Uniqueness of Tetration</title>
		<link rel="alternate" type="text/html" href="https://tetrationforum.org/hyperops_wiki/index.php?title=Uniqueness_of_Tetration&amp;diff=192"/>
		<updated>2017-01-03T18:55:13Z</updated>

		<summary type="html">&lt;p&gt;Bo198214: /* Proof. */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Proposition ==&lt;br /&gt;
For each $b&amp;gt;e^{1/e}$ there exists exactly one holomorphic function $\sigma_b$ on $D=\C\setminus\{x \le -2\}$ which is real for all $x&amp;gt;-2$ and satisfies for all $z\in D$:&lt;br /&gt;
$$\sigma_b(0)=1, \sigma_b(z+1)=b^{\sigma_b(z)}$$ and $$\sup_{t\to\infty}\left| \sigma_b({\rm i}t)\right| &amp;lt;\infty$$.&lt;br /&gt;
&lt;br /&gt;
==== Proof. ====&lt;br /&gt;
We know there exists already a solution $\tau_b$ which satisfies all conditions and its inverse $\alpha_b$ which is a whole function and satisifies $\alpha_b(b^z)=\alpha_b(z)+1$.&lt;br /&gt;
Then we know that &lt;br /&gt;
$$\sup_{t\to\infty}\alpha_b(\sigma_b({\rm i}t))&amp;lt;\infty$$&lt;br /&gt;
and the function $\delta(z)=\alpha_b(\sigma_b(z))-z$, holomorphic on $D$, is periodic with period 1:&lt;br /&gt;
$$\delta(z+1)=(\alpha_b(\sigma_b(z+1))-(z+1)=\alpha_b(\sigma_b(z))-z=\delta_b(z)$$&lt;br /&gt;
and is real for $z &amp;gt; -2$ (and can be continued to $\R$) and can so be developed into a real Fourier-Series ($A_k$,  $\phi_k$ in $\R$):&lt;br /&gt;
&lt;br /&gt;
$$\delta(t)=\sum_{k=0}^{\infty}A_{k}\cos\left(2\pi kt-\varphi_{k}\right)$$&lt;br /&gt;
&lt;br /&gt;
$$\delta(z)=\sum_{k=0}^{\infty}\frac{A_{k}}{2}\left(\exp\left(2\pi {\rm i}kz-{\rm i}\varphi_{k}\right)+\exp\left(-2\pi {\rm i}kz+{\rm i}\varphi_{k}\right)\right)$$&lt;br /&gt;
$$\delta(x+{\rm i}y)=\sum_{k=0}^{\infty}\frac{A_{k}}{2}\left(\exp\left({\rm i}(2\pi kx-\varphi_{k})-2\pi k y\right)+\exp\left({\rm i}(-2\pi kx+\varphi_{k})+2\pi k y\right)\right)&lt;br /&gt;
=\sum_{k=0}^{\infty}\frac{A_{k}}{2}\left(\cos(2\pi kx-\varphi_{k})\left(\exp\left(-2\pi k y\right)+\exp(2\pi ky)\right)+{\rm i}\sin(2\pi kx-\varphi_{k})\left(-\exp\left(2\pi k y\right)+\exp(-2\pi ky)\right)\right)$$&lt;br /&gt;
&lt;br /&gt;
$$\Im(\delta(x+{\rm i}y))=\sum_{k=0}^{\infty}\frac{A_{k}}{2}\sin(2\pi kx-\varphi_{k})\left(-\exp\left(2\pi k y\right)+\exp(-2\pi ky)\right)$$&lt;br /&gt;
&lt;br /&gt;
$$&lt;br /&gt;
\alpha_b(\sigma_b({\rm i}t))=\delta({\rm i}t)+{\rm i}t={\rm i}t+\sum_{k=0}^{\infty}\frac{A_{k}}{2}\left(\exp\left(-2\pi kt -{\rm i}\varphi_{k}\right)+\exp\left(2\pi kt+{\rm i}\varphi_{k}\right)\right)&lt;br /&gt;
$$&lt;br /&gt;
&lt;br /&gt;
But this expression can only be bounded with respect to $t$ if $A_k=0$ for all $k\ge 1$. Hence $\delta$ is a constant $c$ and $\sigma_b(z)=\tau_b(z+c)$.&lt;/div&gt;</summary>
		<author><name>Bo198214</name></author>
	</entry>
	<entry>
		<id>https://tetrationforum.org/hyperops_wiki/index.php?title=Uniqueness_of_Tetration&amp;diff=191</id>
		<title>Uniqueness of Tetration</title>
		<link rel="alternate" type="text/html" href="https://tetrationforum.org/hyperops_wiki/index.php?title=Uniqueness_of_Tetration&amp;diff=191"/>
		<updated>2017-01-03T16:42:42Z</updated>

		<summary type="html">&lt;p&gt;Bo198214: /* Proposition */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Proposition ==&lt;br /&gt;
For each $b&amp;gt;e^{1/e}$ there exists exactly one holomorphic function $\sigma_b$ on $D=\C\setminus\{x \le -2\}$ which is real for all $x&amp;gt;-2$ and satisfies for all $z\in D$:&lt;br /&gt;
$$\sigma_b(0)=1, \sigma_b(z+1)=b^{\sigma_b(z)}$$ and $$\sup_{t\to\infty}\left| \sigma_b({\rm i}t)\right| &amp;lt;\infty$$.&lt;br /&gt;
&lt;br /&gt;
==== Proof. ====&lt;br /&gt;
We know there exists already a solution $\tau_b$ which satisfies all conditions and its inverse $\alpha_b$ which is a whole function and satisifies $\alpha_b(b^z)=\alpha_b(z)+1$.&lt;br /&gt;
Then we know that the function $\delta(z)=\alpha_b(\sigma_b(z))-z$, holomorphic on $D$, is periodic with period 1:&lt;br /&gt;
$$\delta(z+1)=(\alpha_b(\sigma_b(z+1))-(z+1)=\alpha_b(\sigma_b(z))-z=\delta_b(z)$$&lt;br /&gt;
and is real for $z &amp;gt; -2$ (and can be continued to $\R$) and can so be developed into a real Fourier-Series ($A_k$,  $\phi_k$ in $\R$):&lt;br /&gt;
&lt;br /&gt;
$$\delta(t)=\sum_{k=0}^{\infty}A_{k}\cos\left(2\pi kt-\varphi_{k}\right)$$&lt;br /&gt;
&lt;br /&gt;
$$\delta(z)=\sum_{k=0}^{\infty}\frac{A_{k}}{2}\left(\exp\left(2\pi {\rm i}kz-{\rm i}\varphi_{k}\right)+\exp\left(-2\pi {\rm i}kz+{\rm i}\varphi_{k}\right)\right)$$&lt;br /&gt;
&lt;br /&gt;
$$&lt;br /&gt;
\delta({\rm i}t)=\sum_{k=0}^{\infty}\frac{A_{k}}{2}\left(\exp\left(-2\pi kt -{\rm i}\varphi_{k}\right)+\exp\left(2\pi kt+{\rm i}\varphi_{k}\right)\right)&lt;br /&gt;
$$&lt;br /&gt;
&lt;br /&gt;
But this expression can only be bounded with respect to $t$ if $A_k=0$ for all $k\ge 1$. Hence $\delta$ is a constant $c$ and $\sigma_b(z)=\tau_b(z+c)$.&lt;/div&gt;</summary>
		<author><name>Bo198214</name></author>
	</entry>
	<entry>
		<id>https://tetrationforum.org/hyperops_wiki/index.php?title=Uniqueness_of_Tetration&amp;diff=190</id>
		<title>Uniqueness of Tetration</title>
		<link rel="alternate" type="text/html" href="https://tetrationforum.org/hyperops_wiki/index.php?title=Uniqueness_of_Tetration&amp;diff=190"/>
		<updated>2017-01-03T16:25:12Z</updated>

		<summary type="html">&lt;p&gt;Bo198214: /* Proof. */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Proposition ==&lt;br /&gt;
For each $b&amp;gt;e^{1/e}$ there exists exactly one holomorphic function $\sigma_b$ on $D=\C\setminus\{x \le -2\}$ which satisfies for all $z\in D$:&lt;br /&gt;
$$\overline{\sigma_b(z)}=\sigma_b(\overline{z})$$, $$\sigma_b(z+1)=b^{\sigma_b(z)}$$ and $$\sup_{t\to\infty}\left| \sigma_b(s+{\rm i}t)\right| &amp;lt;\infty$$ for each $s&amp;gt;-2$.&lt;br /&gt;
&lt;br /&gt;
==== Proof. ====&lt;br /&gt;
We know there exists already a solution $\tau_b$ which satisfies all conditions and its inverse $\alpha_b$ which is a whole function and satisifies $\alpha_b(b^z)=\alpha_b(z)+1$.&lt;br /&gt;
Then we know that the function $\delta(z)=\alpha_b(\sigma_b(z))-z$, holomorphic on $D$, is periodic with period 1:&lt;br /&gt;
$$\delta(z+1)=(\alpha_b(\sigma_b(z+1))-(z+1)=\alpha_b(\sigma_b(z))-z=\delta_b(z)$$&lt;br /&gt;
and is real for $z &amp;gt; -2$ (and can be continued to $\R$) and can to developed into a real Fourier-Series ($A_k$,  $\phi_k$ in $\R$):&lt;br /&gt;
&lt;br /&gt;
$$\delta(t)=\sum_{k=0}^{\infty}A_{k}\cos\left(2\pi kt-\varphi_{k}\right)$$&lt;br /&gt;
&lt;br /&gt;
$$\delta(z)=\sum_{k=0}^{\infty}\frac{A_{k}}{2}\left(\exp\left(2\pi {\rm i}kz-{\rm i}\varphi_{k}\right)+\exp\left(-2\pi {\rm i}kz+{\rm i}\varphi_{k}\right)\right)$$&lt;br /&gt;
&lt;br /&gt;
$$&lt;br /&gt;
\delta(s+{\rm i}t)=\sum_{k=0}^{\infty}\frac{A_{k}}{2}\left(\exp\left(2\pi {\rm i}ks-2\pi kt -{\rm i}\varphi_{k}\right)+\exp\left(-2\pi {\rm i}ks+2\pi kt+{\rm i}\varphi_{k}\right)\right)&lt;br /&gt;
$$&lt;br /&gt;
&lt;br /&gt;
But this expression can only be bounded with respect to $t$ if $A_k=0$ for all $k\ge 1$. Hence $\delta$ is a constant $c$ and $\sigma_b(z)=\tau_b(z+c)$.&lt;/div&gt;</summary>
		<author><name>Bo198214</name></author>
	</entry>
	<entry>
		<id>https://tetrationforum.org/hyperops_wiki/index.php?title=Uniqueness_of_Tetration&amp;diff=189</id>
		<title>Uniqueness of Tetration</title>
		<link rel="alternate" type="text/html" href="https://tetrationforum.org/hyperops_wiki/index.php?title=Uniqueness_of_Tetration&amp;diff=189"/>
		<updated>2017-01-03T16:20:22Z</updated>

		<summary type="html">&lt;p&gt;Bo198214: Created page with &amp;quot;== Proposition == For each $b&amp;gt;e^{1/e}$ there exists exactly one holomorphic function $\sigma_b$ on $D=\C\setminus\{x \le -2\}$ which satisfies for all $z\in D$: $$\overline{\s...&amp;quot;&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Proposition ==&lt;br /&gt;
For each $b&amp;gt;e^{1/e}$ there exists exactly one holomorphic function $\sigma_b$ on $D=\C\setminus\{x \le -2\}$ which satisfies for all $z\in D$:&lt;br /&gt;
$$\overline{\sigma_b(z)}=\sigma_b(\overline{z})$$, $$\sigma_b(z+1)=b^{\sigma_b(z)}$$ and $$\sup_{t\to\infty}\left| \sigma_b(s+{\rm i}t)\right| &amp;lt;\infty$$ for each $s&amp;gt;-2$.&lt;br /&gt;
&lt;br /&gt;
==== Proof. ====&lt;br /&gt;
We know there exists already a solution $\tau_b$ which satisfies all conditions and its inverse $\alpha_b$ which is a whole function and satisifies $\alpha_b(b^z)=\alpha_b(z)+1$.&lt;br /&gt;
Then we know that the function $\delta(z)=\alpha_b(\sigma_b(z))-z$, holomorphic on $D$, is periodic with period 1:&lt;br /&gt;
$$\delta(z+1)=(\alpha_b(\sigma_b(z+1))-(z+1)=\alpha_b(\sigma_b(z))-z=\delta_b(z)$$&lt;br /&gt;
and is real for $z &amp;gt; -2$ (and can be continued to $\R$) and can to developed into a real Fourier-Series ($A_k$,  $\phi_k$ in $\R$):&lt;br /&gt;
&lt;br /&gt;
$$\delta(t)=\sum_{k=0}^{\infty}A_{k}\cos\left(2\pi kt-\varphi_{k}\right)$$&lt;br /&gt;
&lt;br /&gt;
$$\delta(z)=\sum_{k=0}^{\infty}\frac{A_{k}}{2}\left(\exp\left(2\pi {\rm i}kz-{\rm i}\varphi_{k}\right)+\exp\left(-2\pi {\rm i}kz+{\rm i}\varphi_{k}\right)\right)$$&lt;br /&gt;
&lt;br /&gt;
$$&lt;br /&gt;
\delta(s+{\rm i}t)=\sum_{k=0}^{\infty}\frac{A_{k}}{2}\left(\exp\left(2\pi {\rm i}ks-2\pi kt -{\rm i}\varphi_{k}\right)+\exp\left(-2\pi {\rm i}ks+2\pi kt+{\rm i}\varphi_{k}\right)\right)&lt;br /&gt;
$$&lt;/div&gt;</summary>
		<author><name>Bo198214</name></author>
	</entry>
	<entry>
		<id>https://tetrationforum.org/hyperops_wiki/index.php?title=Schroeder_iterate&amp;diff=180</id>
		<title>Schroeder iterate</title>
		<link rel="alternate" type="text/html" href="https://tetrationforum.org/hyperops_wiki/index.php?title=Schroeder_iterate&amp;diff=180"/>
		<updated>2013-05-01T16:02:59Z</updated>

		<summary type="html">&lt;p&gt;Bo198214: corrected redirect&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;#REDIRECT[[Schröder iterate]]&lt;/div&gt;</summary>
		<author><name>Bo198214</name></author>
	</entry>
	<entry>
		<id>https://tetrationforum.org/hyperops_wiki/index.php?title=Schroeder_iterate&amp;diff=179</id>
		<title>Schroeder iterate</title>
		<link rel="alternate" type="text/html" href="https://tetrationforum.org/hyperops_wiki/index.php?title=Schroeder_iterate&amp;diff=179"/>
		<updated>2013-05-01T16:02:06Z</updated>

		<summary type="html">&lt;p&gt;Bo198214: Weiterleitung&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;#REDIRECT[[Schröder Iterate]]&lt;/div&gt;</summary>
		<author><name>Bo198214</name></author>
	</entry>
	<entry>
		<id>https://tetrationforum.org/hyperops_wiki/index.php?title=Iteration_of_fractional_linear_maps&amp;diff=178</id>
		<title>Iteration of fractional linear maps</title>
		<link rel="alternate" type="text/html" href="https://tetrationforum.org/hyperops_wiki/index.php?title=Iteration_of_fractional_linear_maps&amp;diff=178"/>
		<updated>2013-05-01T15:56:40Z</updated>

		<summary type="html">&lt;p&gt;Bo198214: /* Iterates */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Our concern here are functions of the form $f(z)=\frac{az+b}{cz+d}$ with $c\neq 0$.&lt;br /&gt;
&lt;br /&gt;
== Fixpoints ==&lt;br /&gt;
In the case $c\neq 0$, the fixpoints are given by&lt;br /&gt;
&lt;br /&gt;
$L_{1,2}=-\frac{d-a}{2c} \pm \sqrt{\left(\frac{d-a}{2c}\right)^2 + \frac{b}{c}}$, or for later use:&lt;br /&gt;
&lt;br /&gt;
$cL_{1,2}=-d + a_2 \pm a_2\underbrace{\sqrt{1-\frac{ad-bc}{a_2^2}}}_{=:q}$, where $a_2=\frac{a+d}{2}$.&lt;br /&gt;
&lt;br /&gt;
== Derivative at the fixpoints ==&lt;br /&gt;
&lt;br /&gt;
The derivative of the fractional linear map $f$ is:&lt;br /&gt;
 &lt;br /&gt;
$f&amp;#039;(z)=\frac{ad-bz}{(cz+d)^2}$&lt;br /&gt;
&lt;br /&gt;
If we plug in $z=L_1$ we get:&lt;br /&gt;
&lt;br /&gt;
$f&amp;#039;(L_1) = \frac{ad-bz}{(a_2(1+q))^2} = \frac{ad-bz}{a_2^2}/\left(1+q\right)^2 = \frac{1-q^2}{\left(1+q\right)^2} = \frac{1-q}{1+q}$&lt;br /&gt;
&lt;br /&gt;
$f&amp;#039;(L_2) = \frac{1+q}{1-q} = 1/f&amp;#039;(L_1)$.&lt;br /&gt;
&lt;br /&gt;
== [[Schröder coordinate]] at the fixpoints ==&lt;br /&gt;
&lt;br /&gt;
Let $\sigma_k(f(z))=f&amp;#039;(L_k) \sigma(z)$, $\sigma_k$ is unique up to a multiplicative constant.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Then $\sigma_1(z) = \frac{z-L_1}{z-L_2}$, $\sigma_2(z)=\frac{z-L_2}{z-L_1}$.&lt;br /&gt;
&lt;br /&gt;
=== Proof ===&lt;br /&gt;
&lt;br /&gt;
$\sigma_1\left(\frac{az+b}{cz+d}\right) = \frac{(a-cL_1)z + b-dL_1}{(a-cL_2)z + b -dL_2} = \frac{a_2(1-q)z+b- dL_1}{a_2(1+q)z + b -dL_2 }=\frac{1-q}{1+q}\frac{z-\frac{dL_1-b}{cL_2+d}}{z-\frac{dL_2-b}{cL_1+d}}$.&lt;br /&gt;
&lt;br /&gt;
$c^2 L_1 L_2 = (-d+a_2+a_2 q)(-d+a_2 - a_2 q) = (-d+a_2)^2 - a_2^2 q^2 = \frac{(a-d)^2}{4} - \frac{(a+d)^2}{4} + ad - bc = -bc$&lt;br /&gt;
&lt;br /&gt;
$(cL_2+d)L_1 = -b + dL_1$&lt;br /&gt;
&lt;br /&gt;
$\sigma_1\left(\frac{az+b}{cz+d}\right) = \frac{1-q}{1+q} \frac{z-L_1}{z-L_2} = f&amp;#039;(L_1) \sigma_1(z)$&lt;br /&gt;
&lt;br /&gt;
== Iterates ==&lt;br /&gt;
&lt;br /&gt;
The iterates $f^t$ of $f$ can then be given by: &lt;br /&gt;
&lt;br /&gt;
$f_k^t(z) = \sigma_k^{-1}(f&amp;#039;(L_k)^t \sigma_k(z))$&lt;br /&gt;
&lt;br /&gt;
$\sigma_1^{-1}(w) = \frac{L_2w-L_1}{w-1}$&lt;br /&gt;
&lt;br /&gt;
$f_1^t(z) = \frac{L_2K^t\frac{z-L_1}{z-L_2} - L_1}{K^t\frac{z-L_1}{z-L_2}-1} = \frac{(L_2K^t-L_1)z -L_2K^tL_1 + L_2L_1}{(K^t-1)z+K^tL_1-L_2} = &lt;br /&gt;
\frac{(L_2K^t-L_1)z + (K^t-1)\frac{b}{c}}{(K^t-1)z + K^tL_1 - L_2} = \frac{(L_2 (1-q)^t-L_1 (1+q)^t)z + ((1-q)^t-(1+q)^t)\frac{b}{c}}{((1-q)^t-(1+q)^t)z + (1-q)^tL_1 - (1+q)^tL_2}$&lt;br /&gt;
&lt;br /&gt;
$s_t := (1-q)^t - (1+q)^t$&lt;br /&gt;
&lt;br /&gt;
$f^t(z) = \frac{(-d s_t + a_2 s_{t+1})z + s_t b}{s_t c z - d s_t + a_2 (1-q^2) s_{t-1}} = \frac{(-d+a_2 \frac{s_{t+1}}{s_t})z + b}{cz-d+a_2\frac{(1-q^2)s_{t-1}}{s_t}}$&lt;br /&gt;
&lt;br /&gt;
We see indeed that this is independent of the sign of $q$, i.e. regardless at which fixpoint the iterate is developed, the result is the same.&lt;/div&gt;</summary>
		<author><name>Bo198214</name></author>
	</entry>
	<entry>
		<id>https://tetrationforum.org/hyperops_wiki/index.php?title=Iteration_of_fractional_linear_maps&amp;diff=177</id>
		<title>Iteration of fractional linear maps</title>
		<link rel="alternate" type="text/html" href="https://tetrationforum.org/hyperops_wiki/index.php?title=Iteration_of_fractional_linear_maps&amp;diff=177"/>
		<updated>2013-05-01T15:55:27Z</updated>

		<summary type="html">&lt;p&gt;Bo198214: /* Iterates */ fixed sign error&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Our concern here are functions of the form $f(z)=\frac{az+b}{cz+d}$ with $c\neq 0$.&lt;br /&gt;
&lt;br /&gt;
== Fixpoints ==&lt;br /&gt;
In the case $c\neq 0$, the fixpoints are given by&lt;br /&gt;
&lt;br /&gt;
$L_{1,2}=-\frac{d-a}{2c} \pm \sqrt{\left(\frac{d-a}{2c}\right)^2 + \frac{b}{c}}$, or for later use:&lt;br /&gt;
&lt;br /&gt;
$cL_{1,2}=-d + a_2 \pm a_2\underbrace{\sqrt{1-\frac{ad-bc}{a_2^2}}}_{=:q}$, where $a_2=\frac{a+d}{2}$.&lt;br /&gt;
&lt;br /&gt;
== Derivative at the fixpoints ==&lt;br /&gt;
&lt;br /&gt;
The derivative of the fractional linear map $f$ is:&lt;br /&gt;
 &lt;br /&gt;
$f&amp;#039;(z)=\frac{ad-bz}{(cz+d)^2}$&lt;br /&gt;
&lt;br /&gt;
If we plug in $z=L_1$ we get:&lt;br /&gt;
&lt;br /&gt;
$f&amp;#039;(L_1) = \frac{ad-bz}{(a_2(1+q))^2} = \frac{ad-bz}{a_2^2}/\left(1+q\right)^2 = \frac{1-q^2}{\left(1+q\right)^2} = \frac{1-q}{1+q}$&lt;br /&gt;
&lt;br /&gt;
$f&amp;#039;(L_2) = \frac{1+q}{1-q} = 1/f&amp;#039;(L_1)$.&lt;br /&gt;
&lt;br /&gt;
== [[Schröder coordinate]] at the fixpoints ==&lt;br /&gt;
&lt;br /&gt;
Let $\sigma_k(f(z))=f&amp;#039;(L_k) \sigma(z)$, $\sigma_k$ is unique up to a multiplicative constant.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Then $\sigma_1(z) = \frac{z-L_1}{z-L_2}$, $\sigma_2(z)=\frac{z-L_2}{z-L_1}$.&lt;br /&gt;
&lt;br /&gt;
=== Proof ===&lt;br /&gt;
&lt;br /&gt;
$\sigma_1\left(\frac{az+b}{cz+d}\right) = \frac{(a-cL_1)z + b-dL_1}{(a-cL_2)z + b -dL_2} = \frac{a_2(1-q)z+b- dL_1}{a_2(1+q)z + b -dL_2 }=\frac{1-q}{1+q}\frac{z-\frac{dL_1-b}{cL_2+d}}{z-\frac{dL_2-b}{cL_1+d}}$.&lt;br /&gt;
&lt;br /&gt;
$c^2 L_1 L_2 = (-d+a_2+a_2 q)(-d+a_2 - a_2 q) = (-d+a_2)^2 - a_2^2 q^2 = \frac{(a-d)^2}{4} - \frac{(a+d)^2}{4} + ad - bc = -bc$&lt;br /&gt;
&lt;br /&gt;
$(cL_2+d)L_1 = -b + dL_1$&lt;br /&gt;
&lt;br /&gt;
$\sigma_1\left(\frac{az+b}{cz+d}\right) = \frac{1-q}{1+q} \frac{z-L_1}{z-L_2} = f&amp;#039;(L_1) \sigma_1(z)$&lt;br /&gt;
&lt;br /&gt;
== Iterates ==&lt;br /&gt;
&lt;br /&gt;
The iterates $f^t$ of $f$ can then be given by: &lt;br /&gt;
&lt;br /&gt;
$f_k^t(z) = \sigma_k^{-1}(f&amp;#039;(L_k)^t \sigma_k(z))$&lt;br /&gt;
&lt;br /&gt;
$\sigma_1^{-1}(w) = \frac{L_2w-L_1}{w-1}$&lt;br /&gt;
&lt;br /&gt;
$f_1^t(z) = \frac{L_2K^t\frac{z-L_1}{z-L_2} - L_1}{K^t\frac{z-L_1}{z-L_2}-1} = \frac{(L_2K^t-L_1)z -L_2K^tL_1 + L_2L_1}{(K^t-1)z+K^tL_1-L_2} = &lt;br /&gt;
\frac{(L_2K^t-L_1)z + (K^t-1)\frac{b}{c}}{(K^t-1)z + K^tL_1 - L_2} = \frac{(L_2 (1-q)^t-L_1 (1+q)^t)z + ((1-q)^t-(1+q)^t)\frac{b}{c}}{((1-q)^t-(1+q)^t)z + (1-q)^tL_1 - (1+q)^tL_2}$&lt;br /&gt;
&lt;br /&gt;
$s_t := (1-q)^t - (1+q)^t$&lt;br /&gt;
&lt;br /&gt;
$f^t(z) = \frac{(-d s_t + a_2 s_{t+1})z + s_t b}{s_t c z - d s_t + a_2 (1-q^2) s_{t-1}} = \frac{(-d+a_2 \frac{s_{t+1}}{s_t})z + b}{cz-d+a_2(1-q^2)\frac{s_{t-1}}{s_t}}$&lt;br /&gt;
&lt;br /&gt;
We see indeed that this is independent of the sign of $q$, i.e. regardless at which fixpoint the iterate is developed, the result is the same.&lt;/div&gt;</summary>
		<author><name>Bo198214</name></author>
	</entry>
	<entry>
		<id>https://tetrationforum.org/hyperops_wiki/index.php?title=Iteration_of_fractional_linear_maps&amp;diff=176</id>
		<title>Iteration of fractional linear maps</title>
		<link rel="alternate" type="text/html" href="https://tetrationforum.org/hyperops_wiki/index.php?title=Iteration_of_fractional_linear_maps&amp;diff=176"/>
		<updated>2013-05-01T15:44:28Z</updated>

		<summary type="html">&lt;p&gt;Bo198214: /* Iterates */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Our concern here are functions of the form $f(z)=\frac{az+b}{cz+d}$ with $c\neq 0$.&lt;br /&gt;
&lt;br /&gt;
== Fixpoints ==&lt;br /&gt;
In the case $c\neq 0$, the fixpoints are given by&lt;br /&gt;
&lt;br /&gt;
$L_{1,2}=-\frac{d-a}{2c} \pm \sqrt{\left(\frac{d-a}{2c}\right)^2 + \frac{b}{c}}$, or for later use:&lt;br /&gt;
&lt;br /&gt;
$cL_{1,2}=-d + a_2 \pm a_2\underbrace{\sqrt{1-\frac{ad-bc}{a_2^2}}}_{=:q}$, where $a_2=\frac{a+d}{2}$.&lt;br /&gt;
&lt;br /&gt;
== Derivative at the fixpoints ==&lt;br /&gt;
&lt;br /&gt;
The derivative of the fractional linear map $f$ is:&lt;br /&gt;
 &lt;br /&gt;
$f&amp;#039;(z)=\frac{ad-bz}{(cz+d)^2}$&lt;br /&gt;
&lt;br /&gt;
If we plug in $z=L_1$ we get:&lt;br /&gt;
&lt;br /&gt;
$f&amp;#039;(L_1) = \frac{ad-bz}{(a_2(1+q))^2} = \frac{ad-bz}{a_2^2}/\left(1+q\right)^2 = \frac{1-q^2}{\left(1+q\right)^2} = \frac{1-q}{1+q}$&lt;br /&gt;
&lt;br /&gt;
$f&amp;#039;(L_2) = \frac{1+q}{1-q} = 1/f&amp;#039;(L_1)$.&lt;br /&gt;
&lt;br /&gt;
== [[Schröder coordinate]] at the fixpoints ==&lt;br /&gt;
&lt;br /&gt;
Let $\sigma_k(f(z))=f&amp;#039;(L_k) \sigma(z)$, $\sigma_k$ is unique up to a multiplicative constant.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Then $\sigma_1(z) = \frac{z-L_1}{z-L_2}$, $\sigma_2(z)=\frac{z-L_2}{z-L_1}$.&lt;br /&gt;
&lt;br /&gt;
=== Proof ===&lt;br /&gt;
&lt;br /&gt;
$\sigma_1\left(\frac{az+b}{cz+d}\right) = \frac{(a-cL_1)z + b-dL_1}{(a-cL_2)z + b -dL_2} = \frac{a_2(1-q)z+b- dL_1}{a_2(1+q)z + b -dL_2 }=\frac{1-q}{1+q}\frac{z-\frac{dL_1-b}{cL_2+d}}{z-\frac{dL_2-b}{cL_1+d}}$.&lt;br /&gt;
&lt;br /&gt;
$c^2 L_1 L_2 = (-d+a_2+a_2 q)(-d+a_2 - a_2 q) = (-d+a_2)^2 - a_2^2 q^2 = \frac{(a-d)^2}{4} - \frac{(a+d)^2}{4} + ad - bc = -bc$&lt;br /&gt;
&lt;br /&gt;
$(cL_2+d)L_1 = -b + dL_1$&lt;br /&gt;
&lt;br /&gt;
$\sigma_1\left(\frac{az+b}{cz+d}\right) = \frac{1-q}{1+q} \frac{z-L_1}{z-L_2} = f&amp;#039;(L_1) \sigma_1(z)$&lt;br /&gt;
&lt;br /&gt;
== Iterates ==&lt;br /&gt;
&lt;br /&gt;
The iterates $f^t$ of $f$ can then be given by: &lt;br /&gt;
&lt;br /&gt;
$f_k^t(z) = \sigma_k^{-1}(f&amp;#039;(L_k)^t \sigma_k(z))$&lt;br /&gt;
&lt;br /&gt;
$\sigma_1^{-1}(w) = \frac{L_2w-L_1}{w-1}$&lt;br /&gt;
&lt;br /&gt;
$f_1^t(z) = \frac{L_2K^t\frac{z-L_1}{z-L_2} - L_1}{K^t\frac{z-L_1}{z-L_2}-1} = \frac{(L_2K^t-L_1)z -L_2K^tL_1 + L_2L_1}{(K^t-1)z-K^tL_1+L_2} = &lt;br /&gt;
\frac{(L_2K^t-L_1)z + (K^t-1)\frac{b}{c}}{(K^t-1)z - K^tL_1 + L_2} = \frac{(L_2 (1-q)^t-L_1 (1+q)^t)z + ((1-q)^t-(1+q)^t)\frac{b}{c}}{((1-q)^t-(1+q)^t)z - (1-q)^tL_1 + (1+q)^tL_2}$&lt;br /&gt;
&lt;br /&gt;
$s_t := (1-q)^t - (1+q)^t$&lt;br /&gt;
&lt;br /&gt;
$f^t(z) = \frac{(-d s_t + a_2 s_{t+1})z + s_t b}{s_t c z + d s_t - a_2 (1-q^2) s_{t-1}} = \frac{(-d+a_2 \frac{s_{t+1}}{s_t})z + b}{cz+d-a_2(1-q^2)\frac{s_{t-1}}{s_t}}$&lt;br /&gt;
&lt;br /&gt;
We see indeed that this is independent of the sign of $q$, i.e. regardless at which fixpoint the iterate is developed, the result is the same.&lt;/div&gt;</summary>
		<author><name>Bo198214</name></author>
	</entry>
	<entry>
		<id>https://tetrationforum.org/hyperops_wiki/index.php?title=Iteration_of_fractional_linear_maps&amp;diff=175</id>
		<title>Iteration of fractional linear maps</title>
		<link rel="alternate" type="text/html" href="https://tetrationforum.org/hyperops_wiki/index.php?title=Iteration_of_fractional_linear_maps&amp;diff=175"/>
		<updated>2013-05-01T15:23:56Z</updated>

		<summary type="html">&lt;p&gt;Bo198214: /* Iterates */ finished&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Our concern here are functions of the form $f(z)=\frac{az+b}{cz+d}$ with $c\neq 0$.&lt;br /&gt;
&lt;br /&gt;
== Fixpoints ==&lt;br /&gt;
In the case $c\neq 0$, the fixpoints are given by&lt;br /&gt;
&lt;br /&gt;
$L_{1,2}=-\frac{d-a}{2c} \pm \sqrt{\left(\frac{d-a}{2c}\right)^2 + \frac{b}{c}}$, or for later use:&lt;br /&gt;
&lt;br /&gt;
$cL_{1,2}=-d + a_2 \pm a_2\underbrace{\sqrt{1-\frac{ad-bc}{a_2^2}}}_{=:q}$, where $a_2=\frac{a+d}{2}$.&lt;br /&gt;
&lt;br /&gt;
== Derivative at the fixpoints ==&lt;br /&gt;
&lt;br /&gt;
The derivative of the fractional linear map $f$ is:&lt;br /&gt;
 &lt;br /&gt;
$f&amp;#039;(z)=\frac{ad-bz}{(cz+d)^2}$&lt;br /&gt;
&lt;br /&gt;
If we plug in $z=L_1$ we get:&lt;br /&gt;
&lt;br /&gt;
$f&amp;#039;(L_1) = \frac{ad-bz}{(a_2(1+q))^2} = \frac{ad-bz}{a_2^2}/\left(1+q\right)^2 = \frac{1-q^2}{\left(1+q\right)^2} = \frac{1-q}{1+q}$&lt;br /&gt;
&lt;br /&gt;
$f&amp;#039;(L_2) = \frac{1+q}{1-q} = 1/f&amp;#039;(L_1)$.&lt;br /&gt;
&lt;br /&gt;
== [[Schröder coordinate]] at the fixpoints ==&lt;br /&gt;
&lt;br /&gt;
Let $\sigma_k(f(z))=f&amp;#039;(L_k) \sigma(z)$, $\sigma_k$ is unique up to a multiplicative constant.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Then $\sigma_1(z) = \frac{z-L_1}{z-L_2}$, $\sigma_2(z)=\frac{z-L_2}{z-L_1}$.&lt;br /&gt;
&lt;br /&gt;
=== Proof ===&lt;br /&gt;
&lt;br /&gt;
$\sigma_1\left(\frac{az+b}{cz+d}\right) = \frac{(a-cL_1)z + b-dL_1}{(a-cL_2)z + b -dL_2} = \frac{a_2(1-q)z+b- dL_1}{a_2(1+q)z + b -dL_2 }=\frac{1-q}{1+q}\frac{z-\frac{dL_1-b}{cL_2+d}}{z-\frac{dL_2-b}{cL_1+d}}$.&lt;br /&gt;
&lt;br /&gt;
$c^2 L_1 L_2 = (-d+a_2+a_2 q)(-d+a_2 - a_2 q) = (-d+a_2)^2 - a_2^2 q^2 = \frac{(a-d)^2}{4} - \frac{(a+d)^2}{4} + ad - bc = -bc$&lt;br /&gt;
&lt;br /&gt;
$(cL_2+d)L_1 = -b + dL_1$&lt;br /&gt;
&lt;br /&gt;
$\sigma_1\left(\frac{az+b}{cz+d}\right) = \frac{1-q}{1+q} \frac{z-L_1}{z-L_2} = f&amp;#039;(L_1) \sigma_1(z)$&lt;br /&gt;
&lt;br /&gt;
== Iterates ==&lt;br /&gt;
&lt;br /&gt;
The iterates $f^t$ of $f$ can then be given by: &lt;br /&gt;
&lt;br /&gt;
$f^t(z) = \sigma_k^{-1}(f&amp;#039;(L_k)^t \sigma_k(z))$&lt;br /&gt;
&lt;br /&gt;
$\sigma_1^{-1}(w) = \frac{L_2w-L_1}{w-1}$&lt;br /&gt;
&lt;br /&gt;
$f^t(z) = \frac{L_2K^t\frac{z-L_1}{z-L_2} - L_1}{K^t\frac{z-L_1}{z-L_2}-1} = \frac{(L_2K^t-L_1)z -L_2K^tL_1 + L_2L_1}{(K^t-1)z-K^tL_1+L_2} = &lt;br /&gt;
\frac{(L_2K^t-L_1)z + (K^t-1)\frac{b}{c}}{(K^t-1)z - K^tL_1 + L_2} = \frac{(L_2 (1-q)^t-L_1 (1+q)^t)z + ((1-q)^t-(1+q)^t)\frac{b}{c}}{((1-q)^t-(1+q)^t)z - (1-q)^tL_1 + (1+q)^tL_2}$&lt;br /&gt;
&lt;br /&gt;
$s_t := (1-q)^t - (1+q)^t$&lt;br /&gt;
&lt;br /&gt;
$f^t(z) = \frac{(-d s_t + a_2 s_{t+1})z + s_t b}{s_t c z + d s_t - a_2 (1-q^2) s_{t-1}} = \frac{(-d+a_2 \frac{s_{t+1}}{s_t})z + b}{cz+d-a_2(1-q^2)\frac{s_{t-1}}{s_t}}$&lt;br /&gt;
&lt;br /&gt;
We see indeed that this is independent of the sign of $q$, i.e. regardless at which fixpoint the iterate is developed, the result is the same.&lt;/div&gt;</summary>
		<author><name>Bo198214</name></author>
	</entry>
	<entry>
		<id>https://tetrationforum.org/hyperops_wiki/index.php?title=Iteration_of_fractional_linear_maps&amp;diff=174</id>
		<title>Iteration of fractional linear maps</title>
		<link rel="alternate" type="text/html" href="https://tetrationforum.org/hyperops_wiki/index.php?title=Iteration_of_fractional_linear_maps&amp;diff=174"/>
		<updated>2013-05-01T14:47:17Z</updated>

		<summary type="html">&lt;p&gt;Bo198214: /* Iterates */ intermediate&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Our concern here are functions of the form $f(z)=\frac{az+b}{cz+d}$ with $c\neq 0$.&lt;br /&gt;
&lt;br /&gt;
== Fixpoints ==&lt;br /&gt;
In the case $c\neq 0$, the fixpoints are given by&lt;br /&gt;
&lt;br /&gt;
$L_{1,2}=-\frac{d-a}{2c} \pm \sqrt{\left(\frac{d-a}{2c}\right)^2 + \frac{b}{c}}$, or for later use:&lt;br /&gt;
&lt;br /&gt;
$cL_{1,2}=-d + a_2 \pm a_2\underbrace{\sqrt{1-\frac{ad-bc}{a_2^2}}}_{=:q}$, where $a_2=\frac{a+d}{2}$.&lt;br /&gt;
&lt;br /&gt;
== Derivative at the fixpoints ==&lt;br /&gt;
&lt;br /&gt;
The derivative of the fractional linear map $f$ is:&lt;br /&gt;
 &lt;br /&gt;
$f&amp;#039;(z)=\frac{ad-bz}{(cz+d)^2}$&lt;br /&gt;
&lt;br /&gt;
If we plug in $z=L_1$ we get:&lt;br /&gt;
&lt;br /&gt;
$f&amp;#039;(L_1) = \frac{ad-bz}{(a_2(1+q))^2} = \frac{ad-bz}{a_2^2}/\left(1+q\right)^2 = \frac{1-q^2}{\left(1+q\right)^2} = \frac{1-q}{1+q}$&lt;br /&gt;
&lt;br /&gt;
$f&amp;#039;(L_2) = \frac{1+q}{1-q} = 1/f&amp;#039;(L_1)$.&lt;br /&gt;
&lt;br /&gt;
== [[Schröder coordinate]] at the fixpoints ==&lt;br /&gt;
&lt;br /&gt;
Let $\sigma_k(f(z))=f&amp;#039;(L_k) \sigma(z)$, $\sigma_k$ is unique up to a multiplicative constant.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Then $\sigma_1(z) = \frac{z-L_1}{z-L_2}$, $\sigma_2(z)=\frac{z-L_2}{z-L_1}$.&lt;br /&gt;
&lt;br /&gt;
=== Proof ===&lt;br /&gt;
&lt;br /&gt;
$\sigma_1\left(\frac{az+b}{cz+d}\right) = \frac{(a-cL_1)z + b-dL_1}{(a-cL_2)z + b -dL_2} = \frac{a_2(1-q)z+b- dL_1}{a_2(1+q)z + b -dL_2 }=\frac{1-q}{1+q}\frac{z-\frac{dL_1-b}{cL_2+d}}{z-\frac{dL_2-b}{cL_1+d}}$.&lt;br /&gt;
&lt;br /&gt;
$c^2 L_1 L_2 = (-d+a_2+a_2 q)(-d+a_2 - a_2 q) = (-d+a_2)^2 - a_2^2 q^2 = \frac{(a-d)^2}{4} - \frac{(a+d)^2}{4} + ad - bc = -bc$&lt;br /&gt;
&lt;br /&gt;
$(cL_2+d)L_1 = -b + dL_1$&lt;br /&gt;
&lt;br /&gt;
$\sigma_1\left(\frac{az+b}{cz+d}\right) = \frac{1-q}{1+q} \frac{z-L_1}{z-L_2} = f&amp;#039;(L_1) \sigma_1(z)$&lt;br /&gt;
&lt;br /&gt;
== Iterates ==&lt;br /&gt;
&lt;br /&gt;
The iterates $f^t$ of $f$ can then be given by: &lt;br /&gt;
&lt;br /&gt;
$f^t(z) = \sigma_k^{-1}(f&amp;#039;(L_k)^t \sigma_k(z))$&lt;br /&gt;
&lt;br /&gt;
$\sigma_1^{-1}(w) = \frac{L_2w-L_1}{w-1}$&lt;br /&gt;
&lt;br /&gt;
$f^t(z) = \frac{L_2K^t\frac{z-L_1}{z-L_2} - L_1}{K^t\frac{z-L_1}{z-L_2}-1} = \frac{(L_2K^t-L_1)z -L_2K^tL_1 + L_2L_1}{(K^t-1)z-K^tL_1+L_2} = &lt;br /&gt;
\frac{(L_2K^t-L_1)z + (K^t-1)\frac{b}{c}}{(K^t-1)z - K^tL_1 + L_2} = \frac{(L_2 (1-q)^t-L_1 (1+q)^t)z + ((1-q)^t-(1+q)^t)\frac{b}{c}}{((1-q)^t-(1+q)^t)z - (1-q)^tL_1 + (1+q)^tL_2}$&lt;/div&gt;</summary>
		<author><name>Bo198214</name></author>
	</entry>
	<entry>
		<id>https://tetrationforum.org/hyperops_wiki/index.php?title=Iteration_of_fractional_linear_maps&amp;diff=173</id>
		<title>Iteration of fractional linear maps</title>
		<link rel="alternate" type="text/html" href="https://tetrationforum.org/hyperops_wiki/index.php?title=Iteration_of_fractional_linear_maps&amp;diff=173"/>
		<updated>2013-05-01T14:31:55Z</updated>

		<summary type="html">&lt;p&gt;Bo198214: /* Schröder coordinate at the fixpoints */ save state&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Our concern here are functions of the form $f(z)=\frac{az+b}{cz+d}$ with $c\neq 0$.&lt;br /&gt;
&lt;br /&gt;
== Fixpoints ==&lt;br /&gt;
In the case $c\neq 0$, the fixpoints are given by&lt;br /&gt;
&lt;br /&gt;
$L_{1,2}=-\frac{d-a}{2c} \pm \sqrt{\left(\frac{d-a}{2c}\right)^2 + \frac{b}{c}}$, or for later use:&lt;br /&gt;
&lt;br /&gt;
$cL_{1,2}=-d + a_2 \pm a_2\underbrace{\sqrt{1-\frac{ad-bc}{a_2^2}}}_{=:q}$, where $a_2=\frac{a+d}{2}$.&lt;br /&gt;
&lt;br /&gt;
== Derivative at the fixpoints ==&lt;br /&gt;
&lt;br /&gt;
The derivative of the fractional linear map $f$ is:&lt;br /&gt;
 &lt;br /&gt;
$f&amp;#039;(z)=\frac{ad-bz}{(cz+d)^2}$&lt;br /&gt;
&lt;br /&gt;
If we plug in $z=L_1$ we get:&lt;br /&gt;
&lt;br /&gt;
$f&amp;#039;(L_1) = \frac{ad-bz}{(a_2(1+q))^2} = \frac{ad-bz}{a_2^2}/\left(1+q\right)^2 = \frac{1-q^2}{\left(1+q\right)^2} = \frac{1-q}{1+q}$&lt;br /&gt;
&lt;br /&gt;
$f&amp;#039;(L_2) = \frac{1+q}{1-q} = 1/f&amp;#039;(L_1)$.&lt;br /&gt;
&lt;br /&gt;
== [[Schröder coordinate]] at the fixpoints ==&lt;br /&gt;
&lt;br /&gt;
Let $\sigma_k(f(z))=f&amp;#039;(L_k) \sigma(z)$, $\sigma_k$ is unique up to a multiplicative constant.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Then $\sigma_1(z) = \frac{z-L_1}{z-L_2}$, $\sigma_2(z)=\frac{z-L_2}{z-L_1}$.&lt;br /&gt;
&lt;br /&gt;
=== Proof ===&lt;br /&gt;
&lt;br /&gt;
$\sigma_1\left(\frac{az+b}{cz+d}\right) = \frac{(a-cL_1)z + b-dL_1}{(a-cL_2)z + b -dL_2} = \frac{a_2(1-q)z+b- dL_1}{a_2(1+q)z + b -dL_2 }=\frac{1-q}{1+q}\frac{z-\frac{dL_1-b}{cL_2+d}}{z-\frac{dL_2-b}{cL_1+d}}$.&lt;br /&gt;
&lt;br /&gt;
$c^2 L_1 L_2 = (-d+a_2+a_2 q)(-d+a_2 - a_2 q) = (-d+a_2)^2 - a_2^2 q^2 = \frac{(a-d)^2}{4} - \frac{(a+d)^2}{4} + ad - bc = -bc$&lt;br /&gt;
&lt;br /&gt;
$(cL_2+d)L_1 = -b + dL_1$&lt;br /&gt;
&lt;br /&gt;
$\sigma_1\left(\frac{az+b}{cz+d}\right) = \frac{1-q}{1+q} \frac{z-L_1}{z-L_2} = f&amp;#039;(L_1) \sigma_1(z)$&lt;br /&gt;
&lt;br /&gt;
== Iterates ==&lt;br /&gt;
&lt;br /&gt;
The iterates $f^t$ of $f$ can then be given by: &lt;br /&gt;
&lt;br /&gt;
$f^t(z) = \sigma_k^{-1}(f&amp;#039;(L_k)^t \sigma_k(z))$&lt;br /&gt;
&lt;br /&gt;
$\sigma_1^{-1}(w) = \frac{L_2w-L_1}{w-1}$&lt;br /&gt;
&lt;br /&gt;
$f^t(z) = \frac{L_2K^t\frac{z-L_1}{z-L_2} - L_1}{K^t\frac{z-L_1}{z-L_2}-1} = \frac{(L_2K^t-L_1)z -L_2K^tL_1 + L_2L_1}{(K^t-1)z-K^tL_1+L_2} = $&lt;/div&gt;</summary>
		<author><name>Bo198214</name></author>
	</entry>
	<entry>
		<id>https://tetrationforum.org/hyperops_wiki/index.php?title=Iteration_of_fractional_linear_maps&amp;diff=172</id>
		<title>Iteration of fractional linear maps</title>
		<link rel="alternate" type="text/html" href="https://tetrationforum.org/hyperops_wiki/index.php?title=Iteration_of_fractional_linear_maps&amp;diff=172"/>
		<updated>2013-05-01T13:35:30Z</updated>

		<summary type="html">&lt;p&gt;Bo198214: /* Fixpoints */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Our concern here are functions of the form $f(z)=\frac{az+b}{cz+d}$ with $c\neq 0$.&lt;br /&gt;
&lt;br /&gt;
== Fixpoints ==&lt;br /&gt;
In the case $c\neq 0$, the fixpoints are given by&lt;br /&gt;
&lt;br /&gt;
$L_{1,2}=-\frac{d-a}{2c} \pm \sqrt{\left(\frac{d-a}{2c}\right)^2 + \frac{b}{c}}$, or for later use:&lt;br /&gt;
&lt;br /&gt;
$cL_{1,2}=-d + a_2 \pm a_2\underbrace{\sqrt{1-\frac{ad-bc}{a_2^2}}}_{=:q}$, where $a_2=\frac{a+d}{2}$.&lt;br /&gt;
&lt;br /&gt;
== Derivative at the fixpoints ==&lt;br /&gt;
&lt;br /&gt;
The derivative of the fractional linear map $f$ is:&lt;br /&gt;
 &lt;br /&gt;
$f&amp;#039;(z)=\frac{ad-bz}{(cz+d)^2}$&lt;br /&gt;
&lt;br /&gt;
If we plug in $z=L_1$ we get:&lt;br /&gt;
&lt;br /&gt;
$f&amp;#039;(L_1) = \frac{ad-bz}{(a_2(1+q))^2} = \frac{ad-bz}{a_2^2}/\left(1+q\right)^2 = \frac{1-q^2}{\left(1+q\right)^2} = \frac{1-q}{1+q}$&lt;br /&gt;
&lt;br /&gt;
$f&amp;#039;(L_2) = \frac{1+q}{1-q} = 1/f&amp;#039;(L_1)$.&lt;br /&gt;
&lt;br /&gt;
== [[Schröder coordinate]] at the fixpoints ==&lt;br /&gt;
&lt;br /&gt;
$\sigma_k(f(z))=f&amp;#039;(L_k) \sigma(z)$, $\sigma_k$ is unique up to a multiplicative constant.&lt;br /&gt;
&lt;br /&gt;
$\sigma_1(z) = \frac{z-L_1}{z-L_2}$.&lt;br /&gt;
&lt;br /&gt;
$\sigma_1\left(\frac{az+b}{cz+d}\right) = \frac{(a-cL_2)z + b-dL_2}{(a-cL_1)z + b -dL_2} = \frac{a_2(1-q)z+}{a_2(1+q)z + }$.&lt;/div&gt;</summary>
		<author><name>Bo198214</name></author>
	</entry>
	<entry>
		<id>https://tetrationforum.org/hyperops_wiki/index.php?title=Iteration_of_fractional_linear_maps&amp;diff=171</id>
		<title>Iteration of fractional linear maps</title>
		<link rel="alternate" type="text/html" href="https://tetrationforum.org/hyperops_wiki/index.php?title=Iteration_of_fractional_linear_maps&amp;diff=171"/>
		<updated>2013-05-01T13:34:10Z</updated>

		<summary type="html">&lt;p&gt;Bo198214: /* Fixpoints */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Our concern here are functions of the form $f(z)=\frac{az+b}{cz+d}$ with $c\neq 0$.&lt;br /&gt;
&lt;br /&gt;
== Fixpoints ==&lt;br /&gt;
In the case $c\neq 0$, the fixpoints are given by&lt;br /&gt;
&lt;br /&gt;
$L_{1,2}=-\frac{d-a}{2c} \pm \sqrt{\left(\frac{d-a}{2c}\right)^2 + \frac{b}{c}}$, or for later use:&lt;br /&gt;
&lt;br /&gt;
$cL_{1,2}=a_2-d \pm a_2\underbrace{\sqrt{1-\frac{ad-bc}{a_2^2}}}_{=:q}$, where $a_2=\frac{a+d}{2}$.&lt;br /&gt;
&lt;br /&gt;
== Derivative at the fixpoints ==&lt;br /&gt;
&lt;br /&gt;
The derivative of the fractional linear map $f$ is:&lt;br /&gt;
 &lt;br /&gt;
$f&amp;#039;(z)=\frac{ad-bz}{(cz+d)^2}$&lt;br /&gt;
&lt;br /&gt;
If we plug in $z=L_1$ we get:&lt;br /&gt;
&lt;br /&gt;
$f&amp;#039;(L_1) = \frac{ad-bz}{(a_2(1+q))^2} = \frac{ad-bz}{a_2^2}/\left(1+q\right)^2 = \frac{1-q^2}{\left(1+q\right)^2} = \frac{1-q}{1+q}$&lt;br /&gt;
&lt;br /&gt;
$f&amp;#039;(L_2) = \frac{1+q}{1-q} = 1/f&amp;#039;(L_1)$.&lt;br /&gt;
&lt;br /&gt;
== [[Schröder coordinate]] at the fixpoints ==&lt;br /&gt;
&lt;br /&gt;
$\sigma_k(f(z))=f&amp;#039;(L_k) \sigma(z)$, $\sigma_k$ is unique up to a multiplicative constant.&lt;br /&gt;
&lt;br /&gt;
$\sigma_1(z) = \frac{z-L_1}{z-L_2}$.&lt;br /&gt;
&lt;br /&gt;
$\sigma_1\left(\frac{az+b}{cz+d}\right) = \frac{(a-cL_2)z + b-dL_2}{(a-cL_1)z + b -dL_2} = \frac{a_2(1-q)z+}{a_2(1+q)z + }$.&lt;/div&gt;</summary>
		<author><name>Bo198214</name></author>
	</entry>
	<entry>
		<id>https://tetrationforum.org/hyperops_wiki/index.php?title=Iteration_of_fractional_linear_maps&amp;diff=170</id>
		<title>Iteration of fractional linear maps</title>
		<link rel="alternate" type="text/html" href="https://tetrationforum.org/hyperops_wiki/index.php?title=Iteration_of_fractional_linear_maps&amp;diff=170"/>
		<updated>2013-05-01T13:33:16Z</updated>

		<summary type="html">&lt;p&gt;Bo198214: /* Fixpoints */ elegance&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Our concern here are functions of the form $f(z)=\frac{az+b}{cz+d}$ with $c\neq 0$.&lt;br /&gt;
&lt;br /&gt;
== Fixpoints ==&lt;br /&gt;
In the case $c\neq 0$, the fixpoints are given by&lt;br /&gt;
&lt;br /&gt;
$L_{1,2}=-\frac{d-a}{2c} \pm \sqrt{\left(\frac{d-a}{2c}\right)^2 + \frac{b}{c}}$, or for later use:&lt;br /&gt;
&lt;br /&gt;
$cL_{1,2}=a_2-d \pm \underbrace{\sqrt{1-\frac{ad-bc}{a_2^2}}}_{=:q}$, where $a_2=\frac{a+d}{2}$.&lt;br /&gt;
&lt;br /&gt;
== Derivative at the fixpoints ==&lt;br /&gt;
&lt;br /&gt;
The derivative of the fractional linear map $f$ is:&lt;br /&gt;
 &lt;br /&gt;
$f&amp;#039;(z)=\frac{ad-bz}{(cz+d)^2}$&lt;br /&gt;
&lt;br /&gt;
If we plug in $z=L_1$ we get:&lt;br /&gt;
&lt;br /&gt;
$f&amp;#039;(L_1) = \frac{ad-bz}{(a_2(1+q))^2} = \frac{ad-bz}{a_2^2}/\left(1+q\right)^2 = \frac{1-q^2}{\left(1+q\right)^2} = \frac{1-q}{1+q}$&lt;br /&gt;
&lt;br /&gt;
$f&amp;#039;(L_2) = \frac{1+q}{1-q} = 1/f&amp;#039;(L_1)$.&lt;br /&gt;
&lt;br /&gt;
== [[Schröder coordinate]] at the fixpoints ==&lt;br /&gt;
&lt;br /&gt;
$\sigma_k(f(z))=f&amp;#039;(L_k) \sigma(z)$, $\sigma_k$ is unique up to a multiplicative constant.&lt;br /&gt;
&lt;br /&gt;
$\sigma_1(z) = \frac{z-L_1}{z-L_2}$.&lt;br /&gt;
&lt;br /&gt;
$\sigma_1\left(\frac{az+b}{cz+d}\right) = \frac{(a-cL_2)z + b-dL_2}{(a-cL_1)z + b -dL_2} = \frac{a_2(1-q)z+}{a_2(1+q)z + }$.&lt;/div&gt;</summary>
		<author><name>Bo198214</name></author>
	</entry>
	<entry>
		<id>https://tetrationforum.org/hyperops_wiki/index.php?title=Iteration_of_fractional_linear_maps&amp;diff=169</id>
		<title>Iteration of fractional linear maps</title>
		<link rel="alternate" type="text/html" href="https://tetrationforum.org/hyperops_wiki/index.php?title=Iteration_of_fractional_linear_maps&amp;diff=169"/>
		<updated>2013-05-01T13:32:26Z</updated>

		<summary type="html">&lt;p&gt;Bo198214: /* Fixpoints */ fixed typo&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Our concern here are functions of the form $f(z)=\frac{az+b}{cz+d}$ with $c\neq 0$.&lt;br /&gt;
&lt;br /&gt;
== Fixpoints ==&lt;br /&gt;
In the case $c\neq 0$, the fixpoints are given by&lt;br /&gt;
&lt;br /&gt;
$L_{1,2}=-\frac{d-a}{2c} \pm \sqrt{\left(\frac{d-a}{2c}\right)^2 + \frac{b}{c}}$, or for later use:&lt;br /&gt;
&lt;br /&gt;
$L_{1,2}=\Big(a_2-d \pm \underbrace{\sqrt{1-\frac{ad-bc}{a_2^2}}}_{=:q}\Big)/c$, where $a_2=\frac{a+d}{2}$.&lt;br /&gt;
&lt;br /&gt;
== Derivative at the fixpoints ==&lt;br /&gt;
&lt;br /&gt;
The derivative of the fractional linear map $f$ is:&lt;br /&gt;
 &lt;br /&gt;
$f&amp;#039;(z)=\frac{ad-bz}{(cz+d)^2}$&lt;br /&gt;
&lt;br /&gt;
If we plug in $z=L_1$ we get:&lt;br /&gt;
&lt;br /&gt;
$f&amp;#039;(L_1) = \frac{ad-bz}{(a_2(1+q))^2} = \frac{ad-bz}{a_2^2}/\left(1+q\right)^2 = \frac{1-q^2}{\left(1+q\right)^2} = \frac{1-q}{1+q}$&lt;br /&gt;
&lt;br /&gt;
$f&amp;#039;(L_2) = \frac{1+q}{1-q} = 1/f&amp;#039;(L_1)$.&lt;br /&gt;
&lt;br /&gt;
== [[Schröder coordinate]] at the fixpoints ==&lt;br /&gt;
&lt;br /&gt;
$\sigma_k(f(z))=f&amp;#039;(L_k) \sigma(z)$, $\sigma_k$ is unique up to a multiplicative constant.&lt;br /&gt;
&lt;br /&gt;
$\sigma_1(z) = \frac{z-L_1}{z-L_2}$.&lt;br /&gt;
&lt;br /&gt;
$\sigma_1\left(\frac{az+b}{cz+d}\right) = \frac{(a-cL_2)z + b-dL_2}{(a-cL_1)z + b -dL_2} = \frac{a_2(1-q)z+}{a_2(1+q)z + }$.&lt;/div&gt;</summary>
		<author><name>Bo198214</name></author>
	</entry>
	<entry>
		<id>https://tetrationforum.org/hyperops_wiki/index.php?title=Iteration_of_fractional_linear_maps&amp;diff=168</id>
		<title>Iteration of fractional linear maps</title>
		<link rel="alternate" type="text/html" href="https://tetrationforum.org/hyperops_wiki/index.php?title=Iteration_of_fractional_linear_maps&amp;diff=168"/>
		<updated>2013-05-01T13:30:47Z</updated>

		<summary type="html">&lt;p&gt;Bo198214: /* Fixpoints */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Our concern here are functions of the form $f(z)=\frac{az+b}{cz+d}$ with $c\neq 0$.&lt;br /&gt;
&lt;br /&gt;
== Fixpoints ==&lt;br /&gt;
In the case $c\neq 0$, the fixpoints are given by&lt;br /&gt;
&lt;br /&gt;
$L_{1,2}=-\frac{d-a}{2c} \pm \sqrt{\left(\frac{d-a}{2c}\right)^2 + \frac{b}{c}}$, or for later use:&lt;br /&gt;
&lt;br /&gt;
$L_{1,2}=\frac{a_2-d}{c} \pm \underbrace{\sqrt{1-\frac{ad-bc}{a_2^2}}}_{=:q}\Big)$, where $a_2=\frac{a+d}{2}$.&lt;br /&gt;
&lt;br /&gt;
== Derivative at the fixpoints ==&lt;br /&gt;
&lt;br /&gt;
The derivative of the fractional linear map $f$ is:&lt;br /&gt;
 &lt;br /&gt;
$f&amp;#039;(z)=\frac{ad-bz}{(cz+d)^2}$&lt;br /&gt;
&lt;br /&gt;
If we plug in $z=L_1$ we get:&lt;br /&gt;
&lt;br /&gt;
$f&amp;#039;(L_1) = \frac{ad-bz}{(a_2(1+q))^2} = \frac{ad-bz}{a_2^2}/\left(1+q\right)^2 = \frac{1-q^2}{\left(1+q\right)^2} = \frac{1-q}{1+q}$&lt;br /&gt;
&lt;br /&gt;
$f&amp;#039;(L_2) = \frac{1+q}{1-q} = 1/f&amp;#039;(L_1)$.&lt;br /&gt;
&lt;br /&gt;
== [[Schröder coordinate]] at the fixpoints ==&lt;br /&gt;
&lt;br /&gt;
$\sigma_k(f(z))=f&amp;#039;(L_k) \sigma(z)$, $\sigma_k$ is unique up to a multiplicative constant.&lt;br /&gt;
&lt;br /&gt;
$\sigma_1(z) = \frac{z-L_1}{z-L_2}$.&lt;br /&gt;
&lt;br /&gt;
$\sigma_1\left(\frac{az+b}{cz+d}\right) = \frac{(a-cL_2)z + b-dL_2}{(a-cL_1)z + b -dL_2} = \frac{a_2(1-q)z+}{a_2(1+q)z + }$.&lt;/div&gt;</summary>
		<author><name>Bo198214</name></author>
	</entry>
	<entry>
		<id>https://tetrationforum.org/hyperops_wiki/index.php?title=Iteration_of_fractional_linear_maps&amp;diff=167</id>
		<title>Iteration of fractional linear maps</title>
		<link rel="alternate" type="text/html" href="https://tetrationforum.org/hyperops_wiki/index.php?title=Iteration_of_fractional_linear_maps&amp;diff=167"/>
		<updated>2013-05-01T13:22:03Z</updated>

		<summary type="html">&lt;p&gt;Bo198214: /* Derivative at the fixpoints */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Our concern here are functions of the form $f(z)=\frac{az+b}{cz+d}$ with $c\neq 0$.&lt;br /&gt;
&lt;br /&gt;
== Fixpoints ==&lt;br /&gt;
In the case $c\neq 0$, the fixpoints are given by&lt;br /&gt;
&lt;br /&gt;
$L_{1,2}=-\frac{d-a}{2c} \pm \sqrt{\left(\frac{d-a}{2c}\right)^2 + \frac{b}{c}}$, or for later use:&lt;br /&gt;
&lt;br /&gt;
$L_{1,2}=\frac{a_2}{c} \Big(1\pm \underbrace{\sqrt{1-\frac{ad-bc}{a_2^2}}}_{=:q}\Big)-\frac{d}{c}$, where $a_2=\frac{a+d}{2}$.&lt;br /&gt;
&lt;br /&gt;
== Derivative at the fixpoints ==&lt;br /&gt;
&lt;br /&gt;
The derivative of the fractional linear map $f$ is:&lt;br /&gt;
 &lt;br /&gt;
$f&amp;#039;(z)=\frac{ad-bz}{(cz+d)^2}$&lt;br /&gt;
&lt;br /&gt;
If we plug in $z=L_1$ we get:&lt;br /&gt;
&lt;br /&gt;
$f&amp;#039;(L_1) = \frac{ad-bz}{(a_2(1+q))^2} = \frac{ad-bz}{a_2^2}/\left(1+q\right)^2 = \frac{1-q^2}{\left(1+q\right)^2} = \frac{1-q}{1+q}$&lt;br /&gt;
&lt;br /&gt;
$f&amp;#039;(L_2) = \frac{1+q}{1-q} = 1/f&amp;#039;(L_1)$.&lt;br /&gt;
&lt;br /&gt;
== [[Schröder coordinate]] at the fixpoints ==&lt;br /&gt;
&lt;br /&gt;
$\sigma_k(f(z))=f&amp;#039;(L_k) \sigma(z)$, $\sigma_k$ is unique up to a multiplicative constant.&lt;br /&gt;
&lt;br /&gt;
$\sigma_1(z) = \frac{z-L_1}{z-L_2}$.&lt;br /&gt;
&lt;br /&gt;
$\sigma_1\left(\frac{az+b}{cz+d}\right) = \frac{(a-cL_2)z + b-dL_2}{(a-cL_1)z + b -dL_2} = \frac{a_2(1-q)z+}{a_2(1+q)z + }$.&lt;/div&gt;</summary>
		<author><name>Bo198214</name></author>
	</entry>
	<entry>
		<id>https://tetrationforum.org/hyperops_wiki/index.php?title=Iteration_of_fractional_linear_maps&amp;diff=166</id>
		<title>Iteration of fractional linear maps</title>
		<link rel="alternate" type="text/html" href="https://tetrationforum.org/hyperops_wiki/index.php?title=Iteration_of_fractional_linear_maps&amp;diff=166"/>
		<updated>2013-05-01T13:20:38Z</updated>

		<summary type="html">&lt;p&gt;Bo198214: /* Fixpoints */ fixed error&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Our concern here are functions of the form $f(z)=\frac{az+b}{cz+d}$ with $c\neq 0$.&lt;br /&gt;
&lt;br /&gt;
== Fixpoints ==&lt;br /&gt;
In the case $c\neq 0$, the fixpoints are given by&lt;br /&gt;
&lt;br /&gt;
$L_{1,2}=-\frac{d-a}{2c} \pm \sqrt{\left(\frac{d-a}{2c}\right)^2 + \frac{b}{c}}$, or for later use:&lt;br /&gt;
&lt;br /&gt;
$L_{1,2}=\frac{a_2}{c} \Big(1\pm \underbrace{\sqrt{1-\frac{ad-bc}{a_2^2}}}_{=:q}\Big)-\frac{d}{c}$, where $a_2=\frac{a+d}{2}$.&lt;br /&gt;
&lt;br /&gt;
== Derivative at the fixpoints ==&lt;br /&gt;
&lt;br /&gt;
The derivative of the fractional linear map $f$ is:&lt;br /&gt;
 &lt;br /&gt;
$f&amp;#039;(z)=\frac{ad-bz}{(cz+d)^2}$&lt;br /&gt;
&lt;br /&gt;
If we plug in $z=L_1$ we get:&lt;br /&gt;
&lt;br /&gt;
$f&amp;#039;(L_1) = \frac{ad-bz}{(a_1+a_2 q + d)^2} = \frac{ad-bz}{a_2^2}/\left(1+q\right)^2 = \frac{1-q^2}{\left(1+q\right)^2} = \frac{1-q}{1+q}$&lt;br /&gt;
&lt;br /&gt;
$f&amp;#039;(L_2) = \frac{1+q}{1-q} = 1/f&amp;#039;(L_1)$.&lt;br /&gt;
&lt;br /&gt;
== [[Schröder coordinate]] at the fixpoints ==&lt;br /&gt;
&lt;br /&gt;
$\sigma_k(f(z))=f&amp;#039;(L_k) \sigma(z)$, $\sigma_k$ is unique up to a multiplicative constant.&lt;br /&gt;
&lt;br /&gt;
$\sigma_1(z) = \frac{z-L_1}{z-L_2}$.&lt;br /&gt;
&lt;br /&gt;
$\sigma_1\left(\frac{az+b}{cz+d}\right) = \frac{(a-cL_2)z + b-dL_2}{(a-cL_1)z + b -dL_2} = \frac{a_2(1-q)z+}{a_2(1+q)z + }$.&lt;/div&gt;</summary>
		<author><name>Bo198214</name></author>
	</entry>
	<entry>
		<id>https://tetrationforum.org/hyperops_wiki/index.php?title=Iteration_of_fractional_linear_maps&amp;diff=165</id>
		<title>Iteration of fractional linear maps</title>
		<link rel="alternate" type="text/html" href="https://tetrationforum.org/hyperops_wiki/index.php?title=Iteration_of_fractional_linear_maps&amp;diff=165"/>
		<updated>2013-05-01T13:19:28Z</updated>

		<summary type="html">&lt;p&gt;Bo198214: /* Fixpoints */ more poignant formula&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Our concern here are functions of the form $f(z)=\frac{az+b}{cz+d}$ with $c\neq 0$.&lt;br /&gt;
&lt;br /&gt;
== Fixpoints ==&lt;br /&gt;
In the case $c\neq 0$, the fixpoints are given by&lt;br /&gt;
&lt;br /&gt;
$L_{1,2}=-\frac{d-a}{2c} \pm \sqrt{\left(\frac{d-a}{2c}\right)^2 + \frac{b}{c}}$, or for later use:&lt;br /&gt;
&lt;br /&gt;
$L_{1,2}=\frac{a_2}{c} \Big(1\pm \underbrace{\sqrt{1-\frac{ad-bc}{a_2^2}}}_{=:q}\Big)-d$, where $a_2=\frac{a+d}{2}$.&lt;br /&gt;
&lt;br /&gt;
== Derivative at the fixpoints ==&lt;br /&gt;
&lt;br /&gt;
The derivative of the fractional linear map $f$ is:&lt;br /&gt;
 &lt;br /&gt;
$f&amp;#039;(z)=\frac{ad-bz}{(cz+d)^2}$&lt;br /&gt;
&lt;br /&gt;
If we plug in $z=L_1$ we get:&lt;br /&gt;
&lt;br /&gt;
$f&amp;#039;(L_1) = \frac{ad-bz}{(a_1+a_2 q + d)^2} = \frac{ad-bz}{a_2^2}/\left(1+q\right)^2 = \frac{1-q^2}{\left(1+q\right)^2} = \frac{1-q}{1+q}$&lt;br /&gt;
&lt;br /&gt;
$f&amp;#039;(L_2) = \frac{1+q}{1-q} = 1/f&amp;#039;(L_1)$.&lt;br /&gt;
&lt;br /&gt;
== [[Schröder coordinate]] at the fixpoints ==&lt;br /&gt;
&lt;br /&gt;
$\sigma_k(f(z))=f&amp;#039;(L_k) \sigma(z)$, $\sigma_k$ is unique up to a multiplicative constant.&lt;br /&gt;
&lt;br /&gt;
$\sigma_1(z) = \frac{z-L_1}{z-L_2}$.&lt;br /&gt;
&lt;br /&gt;
$\sigma_1\left(\frac{az+b}{cz+d}\right) = \frac{(a-cL_2)z + b-dL_2}{(a-cL_1)z + b -dL_2} = \frac{a_2(1-q)z+}{a_2(1+q)z + }$.&lt;/div&gt;</summary>
		<author><name>Bo198214</name></author>
	</entry>
	<entry>
		<id>https://tetrationforum.org/hyperops_wiki/index.php?title=Iteration_of_fractional_linear_maps&amp;diff=164</id>
		<title>Iteration of fractional linear maps</title>
		<link rel="alternate" type="text/html" href="https://tetrationforum.org/hyperops_wiki/index.php?title=Iteration_of_fractional_linear_maps&amp;diff=164"/>
		<updated>2013-05-01T13:14:40Z</updated>

		<summary type="html">&lt;p&gt;Bo198214: /* Schröder coordinate at the fixpoints */ started derivation&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Our concern here are functions of the form $f(z)=\frac{az+b}{cz+d}$ with $c\neq 0$.&lt;br /&gt;
&lt;br /&gt;
== Fixpoints ==&lt;br /&gt;
In the case $c\neq 0$, the fixpoints are given by&lt;br /&gt;
&lt;br /&gt;
$L_{1,2}=-\frac{d-a}{2c} \pm \sqrt{\left(\frac{d-a}{2c}\right)^2 + \frac{b}{c}}$, or for later use:&lt;br /&gt;
&lt;br /&gt;
$L_{1,2}=\frac{a_1}{c} \pm \frac{a_2}{c} \underbrace{\sqrt{1-\frac{ad-bc}{a_2^2}}}_{=:q}$, where $a_1=\frac{a-d}{2}$ and $a_2=\frac{a+d}{2}$.&lt;br /&gt;
&lt;br /&gt;
== Derivative at the fixpoints ==&lt;br /&gt;
&lt;br /&gt;
The derivative of the fractional linear map $f$ is:&lt;br /&gt;
 &lt;br /&gt;
$f&amp;#039;(z)=\frac{ad-bz}{(cz+d)^2}$&lt;br /&gt;
&lt;br /&gt;
If we plug in $z=L_1$ we get:&lt;br /&gt;
&lt;br /&gt;
$f&amp;#039;(L_1) = \frac{ad-bz}{(a_1+a_2 q + d)^2} = \frac{ad-bz}{a_2^2}/\left(1+q\right)^2 = \frac{1-q^2}{\left(1+q\right)^2} = \frac{1-q}{1+q}$&lt;br /&gt;
&lt;br /&gt;
$f&amp;#039;(L_2) = \frac{1+q}{1-q} = 1/f&amp;#039;(L_1)$.&lt;br /&gt;
&lt;br /&gt;
== [[Schröder coordinate]] at the fixpoints ==&lt;br /&gt;
&lt;br /&gt;
$\sigma_k(f(z))=f&amp;#039;(L_k) \sigma(z)$, $\sigma_k$ is unique up to a multiplicative constant.&lt;br /&gt;
&lt;br /&gt;
$\sigma_1(z) = \frac{z-L_1}{z-L_2}$.&lt;br /&gt;
&lt;br /&gt;
$\sigma_1\left(\frac{az+b}{cz+d}\right) = \frac{(a-cL_2)z + b-dL_2}{(a-cL_1)z + b -dL_2} = \frac{a_2(1-q)z+}{a_2(1+q)z + }$.&lt;/div&gt;</summary>
		<author><name>Bo198214</name></author>
	</entry>
	<entry>
		<id>https://tetrationforum.org/hyperops_wiki/index.php?title=Iteration_of_fractional_linear_maps&amp;diff=163</id>
		<title>Iteration of fractional linear maps</title>
		<link rel="alternate" type="text/html" href="https://tetrationforum.org/hyperops_wiki/index.php?title=Iteration_of_fractional_linear_maps&amp;diff=163"/>
		<updated>2013-05-01T12:33:44Z</updated>

		<summary type="html">&lt;p&gt;Bo198214: added schroeder stub&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Our concern here are functions of the form $f(z)=\frac{az+b}{cz+d}$ with $c\neq 0$.&lt;br /&gt;
&lt;br /&gt;
== Fixpoints ==&lt;br /&gt;
In the case $c\neq 0$, the fixpoints are given by&lt;br /&gt;
&lt;br /&gt;
$L_{1,2}=-\frac{d-a}{2c} \pm \sqrt{\left(\frac{d-a}{2c}\right)^2 + \frac{b}{c}}$, or for later use:&lt;br /&gt;
&lt;br /&gt;
$L_{1,2}=\frac{a_1}{c} \pm \frac{a_2}{c} \underbrace{\sqrt{1-\frac{ad-bc}{a_2^2}}}_{=:q}$, where $a_1=\frac{a-d}{2}$ and $a_2=\frac{a+d}{2}$.&lt;br /&gt;
&lt;br /&gt;
== Derivative at the fixpoints ==&lt;br /&gt;
&lt;br /&gt;
The derivative of the fractional linear map $f$ is:&lt;br /&gt;
 &lt;br /&gt;
$f&amp;#039;(z)=\frac{ad-bz}{(cz+d)^2}$&lt;br /&gt;
&lt;br /&gt;
If we plug in $z=L_1$ we get:&lt;br /&gt;
&lt;br /&gt;
$f&amp;#039;(L_1) = \frac{ad-bz}{(a_1+a_2 q + d)^2} = \frac{ad-bz}{a_2^2}/\left(1+q\right)^2 = \frac{1-q^2}{\left(1+q\right)^2} = \frac{1-q}{1+q}$&lt;br /&gt;
&lt;br /&gt;
$f&amp;#039;(L_2) = \frac{1+q}{1-q} = 1/f&amp;#039;(L_1)$.&lt;br /&gt;
&lt;br /&gt;
== [[Schröder coordinate]] at the fixpoints ==&lt;br /&gt;
&lt;br /&gt;
$\sigma_k(f(z))=f&amp;#039;(L_k) \sigma(z)$.&lt;br /&gt;
&lt;br /&gt;
$\sigma_1(z) = \frac{z-L_1}{z-L_2}$.&lt;/div&gt;</summary>
		<author><name>Bo198214</name></author>
	</entry>
	<entry>
		<id>https://tetrationforum.org/hyperops_wiki/index.php?title=Iteration_of_fractional_linear_maps&amp;diff=162</id>
		<title>Iteration of fractional linear maps</title>
		<link rel="alternate" type="text/html" href="https://tetrationforum.org/hyperops_wiki/index.php?title=Iteration_of_fractional_linear_maps&amp;diff=162"/>
		<updated>2013-05-01T12:27:04Z</updated>

		<summary type="html">&lt;p&gt;Bo198214: /* Derivative at the fixpoints */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Our concern here are functions of the form $f(z)=\frac{az+b}{cz+d}$ with $c\neq 0$.&lt;br /&gt;
&lt;br /&gt;
== Fixpoints ==&lt;br /&gt;
In the case $c\neq 0$, the fixpoints are given by&lt;br /&gt;
&lt;br /&gt;
$L_{1,2}=-\frac{d-a}{2c} \pm \sqrt{\left(\frac{d-a}{2c}\right)^2 + \frac{b}{c}}$, or for later use:&lt;br /&gt;
&lt;br /&gt;
$L_{1,2}=\frac{a_1}{c} \pm \frac{a_2}{c} \underbrace{\sqrt{1-\frac{ad-bc}{a_2^2}}}_{=:q}$, where $a_1=\frac{a-d}{2}$ and $a_2=\frac{a+d}{2}$.&lt;br /&gt;
&lt;br /&gt;
== Derivative at the fixpoints ==&lt;br /&gt;
&lt;br /&gt;
The derivative of the fractional linear map $f$ is:&lt;br /&gt;
 &lt;br /&gt;
$f&amp;#039;(z)=\frac{ad-bz}{(cz+d)^2}$&lt;br /&gt;
&lt;br /&gt;
If we plug in $z=L_1$ we get:&lt;br /&gt;
&lt;br /&gt;
$f&amp;#039;(L_1) = \frac{ad-bz}{(a_1+a_2 q + d)^2} = \frac{ad-bz}{a_2^2}/\left(1+q\right)^2 = \frac{1-q^2}{\left(1+q\right)^2} = \frac{1-q}{1+q}$&lt;br /&gt;
&lt;br /&gt;
$f&amp;#039;(L_2) = \frac{1+q}{1-q} = 1/f&amp;#039;(L_1)$.&lt;/div&gt;</summary>
		<author><name>Bo198214</name></author>
	</entry>
	<entry>
		<id>https://tetrationforum.org/hyperops_wiki/index.php?title=Iteration_of_fractional_linear_maps&amp;diff=161</id>
		<title>Iteration of fractional linear maps</title>
		<link rel="alternate" type="text/html" href="https://tetrationforum.org/hyperops_wiki/index.php?title=Iteration_of_fractional_linear_maps&amp;diff=161"/>
		<updated>2013-05-01T12:26:24Z</updated>

		<summary type="html">&lt;p&gt;Bo198214: added c neq 0 condition&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Our concern here are functions of the form $f(z)=\frac{az+b}{cz+d}$ with $c\neq 0$.&lt;br /&gt;
&lt;br /&gt;
== Fixpoints ==&lt;br /&gt;
In the case $c\neq 0$, the fixpoints are given by&lt;br /&gt;
&lt;br /&gt;
$L_{1,2}=-\frac{d-a}{2c} \pm \sqrt{\left(\frac{d-a}{2c}\right)^2 + \frac{b}{c}}$, or for later use:&lt;br /&gt;
&lt;br /&gt;
$L_{1,2}=\frac{a_1}{c} \pm \frac{a_2}{c} \underbrace{\sqrt{1-\frac{ad-bc}{a_2^2}}}_{=:q}$, where $a_1=\frac{a-d}{2}$ and $a_2=\frac{a+d}{2}$.&lt;br /&gt;
&lt;br /&gt;
== Derivative at the fixpoints ==&lt;br /&gt;
&lt;br /&gt;
The derivative of the fractional linear map $f$ is:&lt;br /&gt;
 &lt;br /&gt;
$f&amp;#039;(z)=\frac{ad-bz}{(cz+d)^2}$&lt;br /&gt;
&lt;br /&gt;
If we plug in $z=L_1$ we get:&lt;br /&gt;
&lt;br /&gt;
$f&amp;#039;(L_1) = \frac{ad-bz}{(a_1+a_2 q + d)^2} = \frac{ad-bz}{a_2^2}/\left(1+q\right)^2 = \frac{1-q^2}{\left(1+q\right)^2} = \frac{1-q}{1+q}$&lt;br /&gt;
&lt;br /&gt;
$f&amp;#039;(L_2) = \frac{1+q}{1-q}$.&lt;/div&gt;</summary>
		<author><name>Bo198214</name></author>
	</entry>
	<entry>
		<id>https://tetrationforum.org/hyperops_wiki/index.php?title=Iteration_of_fractional_linear_maps&amp;diff=160</id>
		<title>Iteration of fractional linear maps</title>
		<link rel="alternate" type="text/html" href="https://tetrationforum.org/hyperops_wiki/index.php?title=Iteration_of_fractional_linear_maps&amp;diff=160"/>
		<updated>2013-05-01T12:24:30Z</updated>

		<summary type="html">&lt;p&gt;Bo198214: finished with derivative formula at fixpoint&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Our concern here are functions of the form $f(z)=\frac{az+b}{cz+d}$.&lt;br /&gt;
&lt;br /&gt;
== Fixpoints ==&lt;br /&gt;
In the case $c\neq 0$, the fixpoints are given by&lt;br /&gt;
&lt;br /&gt;
$L_{1,2}=-\frac{d-a}{2c} \pm \sqrt{\left(\frac{d-a}{2c}\right)^2 + \frac{b}{c}}$, or for later use:&lt;br /&gt;
&lt;br /&gt;
$L_{1,2}=\frac{a_1}{c} \pm \frac{a_2}{c} \underbrace{\sqrt{1-\frac{ad-bc}{a_2^2}}}_{=:q}$, where $a_1=\frac{a-d}{2}$ and $a_2=\frac{a+d}{2}$.&lt;br /&gt;
&lt;br /&gt;
== Derivative at the fixpoints ==&lt;br /&gt;
&lt;br /&gt;
The derivative of the fractional linear map $f$ is:&lt;br /&gt;
 &lt;br /&gt;
$f&amp;#039;(z)=\frac{ad-bz}{(cz+d)^2}$&lt;br /&gt;
&lt;br /&gt;
If we plug in $z=L_1$ we get:&lt;br /&gt;
&lt;br /&gt;
$f&amp;#039;(L_1) = \frac{ad-bz}{(a_1+a_2 q + d)^2} = \frac{ad-bz}{a_2^2}/\left(1+q\right)^2 = \frac{1-q^2}{\left(1+q\right)^2} = \frac{1-q}{1+q}$&lt;br /&gt;
&lt;br /&gt;
$f&amp;#039;(L_2) = \frac{1+q}{1-q}$.&lt;/div&gt;</summary>
		<author><name>Bo198214</name></author>
	</entry>
	<entry>
		<id>https://tetrationforum.org/hyperops_wiki/index.php?title=Fixpoint&amp;diff=159</id>
		<title>Fixpoint</title>
		<link rel="alternate" type="text/html" href="https://tetrationforum.org/hyperops_wiki/index.php?title=Fixpoint&amp;diff=159"/>
		<updated>2013-05-01T11:57:01Z</updated>

		<summary type="html">&lt;p&gt;Bo198214: added example&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;A fixpoint $p$ of a function $f$ is a value such that $f(p)=p$.&lt;br /&gt;
&lt;br /&gt;
If $f$ is a holomorphic function, we define the multiplicity of the fixpoint $p$ to be the [http://en.wikipedia.org/wiki/Zero_(complex_analysis) multiplicity of the zero] of $f(z)-z$ at $p$.&lt;br /&gt;
&lt;br /&gt;
For example $z+z^2$ has multiplicity 2 at fixpoint 0, $2z+z^2$ has multiplicity 1 at fixpoint 0.&lt;/div&gt;</summary>
		<author><name>Bo198214</name></author>
	</entry>
	<entry>
		<id>https://tetrationforum.org/hyperops_wiki/index.php?title=Fixpoint&amp;diff=158</id>
		<title>Fixpoint</title>
		<link rel="alternate" type="text/html" href="https://tetrationforum.org/hyperops_wiki/index.php?title=Fixpoint&amp;diff=158"/>
		<updated>2013-05-01T11:53:20Z</updated>

		<summary type="html">&lt;p&gt;Bo198214: linkt to wikipedia&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;A fixpoint $p$ of a function $f$ is a value such that $f(p)=p$.&lt;br /&gt;
&lt;br /&gt;
If $f$ is a holomorphic function, we define the multiplicity of the fixpoint $p$ to be the [http://en.wikipedia.org/wiki/Zero_(complex_analysis) multiplicity of the zero] of $f(z)-z$ at $p$.&lt;/div&gt;</summary>
		<author><name>Bo198214</name></author>
	</entry>
	<entry>
		<id>https://tetrationforum.org/hyperops_wiki/index.php?title=Fixpoint&amp;diff=157</id>
		<title>Fixpoint</title>
		<link rel="alternate" type="text/html" href="https://tetrationforum.org/hyperops_wiki/index.php?title=Fixpoint&amp;diff=157"/>
		<updated>2013-05-01T11:51:13Z</updated>

		<summary type="html">&lt;p&gt;Bo198214: Added multiplicity.&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;A fixpoint $p$ of a function $f$ is a value such that $f(p)=p$.&lt;br /&gt;
&lt;br /&gt;
If $f$ is a holomorphic function, we define the multiplicity of the fixpoint $p$ to be the multiplicity of the zero of $f(z)-z$ at $p$.&lt;/div&gt;</summary>
		<author><name>Bo198214</name></author>
	</entry>
	<entry>
		<id>https://tetrationforum.org/hyperops_wiki/index.php?title=Shishikura_perturbed_Fatou_coordinates&amp;diff=156</id>
		<title>Shishikura perturbed Fatou coordinates</title>
		<link rel="alternate" type="text/html" href="https://tetrationforum.org/hyperops_wiki/index.php?title=Shishikura_perturbed_Fatou_coordinates&amp;diff=156"/>
		<updated>2013-02-19T21:52:44Z</updated>

		<summary type="html">&lt;p&gt;Bo198214: /* Proposition 3.2.2 */ used wiki numbering&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Shishikura writes&amp;lt;ref name=&amp;quot;Shishikura2000&amp;quot;&amp;gt;Shishikura, M. (2000). Bifurcation of parabolic fixed points. In Lei, Tan, The Mandelbrot set, theme and variations. Cambridge: Cambridge University Press. Lond. Math. Soc. Lect. Note Ser. 274, 325-363 (2000)&amp;lt;/ref&amp;gt; the following&lt;br /&gt;
&lt;br /&gt;
== $\mathcal{F}_0$ ==&lt;br /&gt;
&amp;amp;#91;p. 327&amp;amp;#93;&lt;br /&gt;
 &lt;br /&gt;
If $f_0&amp;#039;&amp;#039;(0)\neq 0$ by another coordinate change we may assume that $f_0&amp;#039;&amp;#039;(0)=1$, so define&lt;br /&gt;
$$ \mathcal{F}_0 = \{ f_0 \colon f_0 \quad\text{is defined and analytic in a neighborhood of 0}\quad f_0(0)=0, f_0&amp;#039;(0)=1, f_0&amp;#039;&amp;#039;(0)=1\}$$&lt;br /&gt;
&lt;br /&gt;
== Neighborhood of $f$ in the compact-open topology with domain of definition ==&lt;br /&gt;
&amp;amp;#91; p. 332 &amp;amp;#93;&lt;br /&gt;
&lt;br /&gt;
In what follows a map $f$ is always associated with its domain of definition $D(f)$. That is two maps are considered as distinct if they have distinct domains, even if the one is an extension of the other. A neighborhood of an analytic map $f\colon D(f)\to\overline{\C}$ is a set containing&lt;br /&gt;
$$\{ g \colon g \quad\text{is analytic},\quad D(g)\supset K, \sup_{z\in K} d(f(z)-g(z))&amp;lt;\eps \} $$&lt;br /&gt;
where $K$ is a compact set in $D(f)$, $\eps&amp;gt;0$ and $d(.,.)$ is the spherical metric.&lt;br /&gt;
A sequence $(f_n)$ converges to $f$ in this topology if and only if for any compact set $K\subset D(f)$ there exists $n_0$ such that $K\subset D(f_n)$ for all $n\ge n_0$ and $f_n|_K\to f|_K$ uniformly on $K$ as $n\to\infty$. The system of these neighborhoods define the &amp;quot;compact-open topology together with the domain of defintion&amp;quot;, which is unfortunately not Hausdorff, since an extension of $f$ is contained in any neighborhood of $f$.&lt;br /&gt;
&lt;br /&gt;
For $b_1,b_2\in\C$ with $\Re(b_1)&amp;lt;\Re(b_2)$ define &lt;br /&gt;
$$Q(b_1,b_2)=\{z\in\C\colon \Re(z-b_1)&amp;gt;-|\Im(z-b_1)|, \Re(z-b_2)&amp;gt;|\Im(z-b_2)|\}$$&lt;br /&gt;
If $b_1=-\infty$ (resp. $b_2=\infty$) then the corresponding condition should be removed.&lt;br /&gt;
&lt;br /&gt;
== Proposition 2.5.2 ==&lt;br /&gt;
&amp;amp;#91;p. 333&amp;amp;#93;&lt;br /&gt;
&lt;br /&gt;
Let $f$ be a holomorphic function defined on $Q=Q(b_1,b_2)$ with $\Re(b_2)&amp;gt;\Re(b_1)+2$ (here $b_1$ or $b_2$ may be $-\infty$ or $\infty$). Suppose &lt;br /&gt;
$$|F(z)-(z+1)|&amp;lt;\frac{1}{4},\quad |F&amp;#039;(z)-(z+1)|&amp;lt;\frac{1}{4}\quad \text{for all}\quad z\in Q.$$&lt;br /&gt;
&lt;br /&gt;
Then&lt;br /&gt;
# $F$ is univalent &amp;amp;#91;means injective&amp;amp;#93; on $Q$.&lt;br /&gt;
# Let $z_0\in Q$ be a point such that $\Re(b_1)&amp;lt;\Re(z_0)&amp;lt;\Re(b_2)-\frac{5}{4}$. Denote by $S$ the closed region (a strip) bounded by the two curves $\ell=\{z_0+i y\colon y\in\R\}$ and $F(\ell)$. Then for any $z\in Q$ there exist a unique $n\in \Z$ such that $F^n(z)$ is defined and belongs to $S-F(\ell)$.&lt;br /&gt;
# There exists an univalent function $\Phi\colon Q\to \C$ satisfying $$\Phi(F(z))=\Phi(z)+1$$ whenever both sides are defined. Moreover $\Phi$ is unique up to an addition of a constant.&lt;br /&gt;
# Fix a point $z_0\in Q$. If we normalize $\Phi$ by $\Phi(z_0)=0$ then the correspondence $F\mapsto \Phi$ is continuous with respect to the compact-open topology.&lt;br /&gt;
&lt;br /&gt;
== $\mathcal{F}$, $\mathcal{F}_1$ and $\alpha(f)$ ==&lt;br /&gt;
&amp;amp;#91;p. 339&amp;amp;#93;&lt;br /&gt;
&lt;br /&gt;
$$ \mathcal{F} = \{ f \colon f \quad\text{is defined and analytic in a neighborhood of 0}\quad f(0)=0, f_0&amp;#039;(0)\neq 0\}$$&lt;br /&gt;
For $f\in \mathcal{F}$ we express the derivative &lt;br /&gt;
$$f&amp;#039;(0)=\exp(2\pi i \alpha(f))$$&lt;br /&gt;
where $\alpha(f)\in\C$ and $-\frac{1}{2} &amp;lt; \Re(\alpha(f)) \le \frac{1}{2}$ our study is focussed on the maps in the following class&lt;br /&gt;
$$ \mathcal{F}_1 = \{ f\in \mathcal{F}\colon |\arg(\alpha(f))| &amp;lt; \frac{\pi}{4}\} $$&lt;br /&gt;
&lt;br /&gt;
=== Comments ===&lt;br /&gt;
&lt;br /&gt;
By the definition we have $$&lt;br /&gt;
\begin{align*}&lt;br /&gt;
\log(f&amp;#039;(0))&amp;amp;=2\pi i\alpha(f)=2\pi i re^{i\beta}=2\pi r e^{i(\beta+\frac{\pi}{2})}\\&lt;br /&gt;
\arg(\log(f&amp;#039;(0))&amp;amp;=\beta+\frac{\pi}{2}&lt;br /&gt;
\end{align*}$$&lt;br /&gt;
so the condition for $\mathcal{F}_1$ is&lt;br /&gt;
$|\arg(\log(f&amp;#039;(0)))-\frac{\pi}{2}|&amp;lt;\frac{\pi}{4}$ or&lt;br /&gt;
$$\frac{\pi}{4} &amp;lt; \arg(\log(f&amp;#039;(0)) &amp;lt; \frac{3\pi}{4}$$&lt;br /&gt;
&lt;br /&gt;
== $\sigma(f)$ ==&lt;br /&gt;
&amp;amp;#91;p. 340&amp;amp;#93;&lt;br /&gt;
&lt;br /&gt;
Let $\sigma(f)$ be the other fixpoint of $f$ (besides 0).&lt;br /&gt;
&lt;br /&gt;
...&lt;br /&gt;
&lt;br /&gt;
$$\sigma(f) = 2\pi i \alpha(f)(1+o(1)), \quad\text{as}\quad f\to f_0$$&lt;br /&gt;
&lt;br /&gt;
=== Comments ===&lt;br /&gt;
&lt;br /&gt;
By the comment before, we can say that $\sigma(f)$ lies roughly in the sector of angle $(\frac{\pi}{4},\frac{3\pi}{4})$ above the tip 0.&lt;br /&gt;
&lt;br /&gt;
== Proposition 3.2.2 ==&lt;br /&gt;
[p. 340]&lt;br /&gt;
&lt;br /&gt;
Let $f_0\in\mathcal{F}_0$. There exists a neighborhood $\mathcal{N}_0$ of $f_0$ (in the sense of the topology defined in 2.5.1) such that if $f\in\mathcal{N}_0\cap \mathcal{F}_1$, then there exist closed Jordan domains $S_{-,f}$, $S_{+,f}$ and analytic functions $\Phi_{-,f}$, $\Phi_{+,f}$ satisfying the following:&lt;br /&gt;
&lt;br /&gt;
# $S_{+,f}$ is bounded by an arc $\ell_{\pm}$ and its image $f(\ell_{\pm})$ such that $\ell_{\pm}$ joins two fixed points $\{0,\sigma(f)\}$, $\ell_{\pm}\cap f(\ell_{\pm}) = \{0,\sigma(f)\}$ and $S_{-,f}\cap S_{+,f} = \{0,\sigma(f)\}$; &lt;br /&gt;
# $\Phi_{\pm,f}$ is defined, analytic and injective in a neighborhood of $S&amp;#039;_{\pm,f} = S_{\pm,f}\setminus \{0,\sigma(f)\}$;&lt;br /&gt;
# if $z\in S&amp;#039;_{-,f}$ then there is an $n\ge 1$ such that $f^n(z)\in S&amp;#039;_{+,f}$ and for the smallest such $n$, \[ \Phi_{+,f}(f^n(z)) = \Phi_{-,f}(z) - \frac{1}{\alpha(f)} + n \]&lt;br /&gt;
# when $f\in\mathcal{F}_1$ tends to $f_0$, $S_{\pm,f}\to S_{\pm,0}\cup \{0\}$ in the Hausdorff metric, and $\Phi_{\pm,f}\to \Phi_{\pm,0}$ in the topology defined in 2.5.1.&lt;br /&gt;
&lt;br /&gt;
== Proposition 4.4.1 ==&lt;br /&gt;
&amp;amp;#91;p. 356&amp;amp;#93;&lt;br /&gt;
&lt;br /&gt;
Let $f_0\in\mathcal{F}_0$, there exists a neighborhood $\mathcal{N}_0$ of $f_0$ (in the previously described &amp;quot;compact-open topology with domain of definition&amp;quot;), such that if $f\in \mathcal{N}_0 \cap \mathcal{F}_1$, then there exist large $\xi_0, \eta_0&amp;gt;0$, and analytic maps $\ph_f\colon D(\ph_f)\to\overline{\C}$ and $\tilde{\mathcal{R}}_f\colon D(\tilde{\mathcal{R}}_f)\to \C$ satisfying the following:&lt;br /&gt;
# $D(\ph_f)$ contains the set $$ \mathcal{Q}_f = \{ w\in\C\colon |\arg(-w-\xi_0)| &amp;lt; \frac{2\pi}{3}, |\arg(w+\frac{1}{\alpha(f)}-\xi_0)|&amp;lt;\frac{2\pi}{3} \} $$ and $\ph_f(D(\ph_f)) \subseteq D(f)$; If $w, w+1\in D(\ph_f)$ then $$ \ph_f(w+1)=f(\ph_f(w)) $$ $\ph_f(w)\to 0$ when $w\in \mathcal{Q}_f$ and $\Im(w)\to\infty$; $\ph_f(w)\to\sigma(f)$ when $w\in\mathcal{Q}_f$ and $\Im(w)\to -\infty$.&lt;br /&gt;
# $D(\tilde{\mathcal{R}}_f)$ contains $\{ w\in\C\colon |\Im(w)| &amp;gt; \eta_0\}$ and is invariant under $T(w)=w+1$; if $w\in D(\tilde{\mathcal{R}}_f)$ then $$\tilde{\mathcal{R}}_f(w+1)=\tilde{\mathcal{R}}(w)+1;$$ $\tilde{\mathcal{R}}_f(w)-w$ tends to $-\frac{1}{\alpha(f)}$ when $\Im(w)\to\infty$; to a constant when $\Im(w)\to -\infty$.&lt;br /&gt;
# If $w\in D(\tilde{\mathcal{R}}_f)\cap D(\ph_f)$ and $w&amp;#039;=\tilde{\mathcal{R}}_f(w)+n\in D(\ph_f)$ for some $n\in\Z$ then $$f^n(\ph_f(w))=\ph_f(w&amp;#039;)\quad \text{for}\quad n\ge 0, \quad f^{-n}(\ph_f(w&amp;#039;))=\ph_f(w)\quad \text{for}\quad n&amp;lt;0$$ Moreover if $|\arg(w&amp;#039;+\frac{1}{2\alpha(f)}-\xi_0)|&amp;lt;\frac{2\pi}{3}$ then $n&amp;gt;0$.&lt;br /&gt;
# When $f\in\mathcal{F_1}$ and $f\to f_0$ $$\ph_f\to\ph_0\quad\text{and}\quad \tilde{\mathcal{R}}_f + \frac{1}{\alpha(f)} \to \tilde{\mathcal{E}}_{f_0}$$&lt;br /&gt;
&lt;br /&gt;
== Proposition A.1 ==&lt;br /&gt;
[p. 360]&lt;br /&gt;
&lt;br /&gt;
In the settings of Proposition 3.2.2 (resp. 2.5.2), assume in addtion that $f_s(z)$ (resp. $F_s(z)$) is a family of holomorphic maps for $s\in \Delta \cup \{0\} \subset \mathbb{C}^k$, with $\Delta\subset\mathbb{C}^k$ an open connected set containing 0 in the boundary, such that $f_s$ (resp. $F_s(z)$) is continuous for $s\in\Delta\cup \{0\}$ and analytic in $s\in\Delta$, then the Fatou coordinates $\Phi_{\pm,f_s}$ (resp. $\Phi_{F_s}$) depend analytically on $s$ for $s\in\Delta$.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;references/&amp;gt;&lt;/div&gt;</summary>
		<author><name>Bo198214</name></author>
	</entry>
	<entry>
		<id>https://tetrationforum.org/hyperops_wiki/index.php?title=Shishikura_perturbed_Fatou_coordinates&amp;diff=155</id>
		<title>Shishikura perturbed Fatou coordinates</title>
		<link rel="alternate" type="text/html" href="https://tetrationforum.org/hyperops_wiki/index.php?title=Shishikura_perturbed_Fatou_coordinates&amp;diff=155"/>
		<updated>2013-02-19T21:50:33Z</updated>

		<summary type="html">&lt;p&gt;Bo198214: /* Proposition A.1 */ added page&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Shishikura writes&amp;lt;ref name=&amp;quot;Shishikura2000&amp;quot;&amp;gt;Shishikura, M. (2000). Bifurcation of parabolic fixed points. In Lei, Tan, The Mandelbrot set, theme and variations. Cambridge: Cambridge University Press. Lond. Math. Soc. Lect. Note Ser. 274, 325-363 (2000)&amp;lt;/ref&amp;gt; the following&lt;br /&gt;
&lt;br /&gt;
== $\mathcal{F}_0$ ==&lt;br /&gt;
&amp;amp;#91;p. 327&amp;amp;#93;&lt;br /&gt;
 &lt;br /&gt;
If $f_0&amp;#039;&amp;#039;(0)\neq 0$ by another coordinate change we may assume that $f_0&amp;#039;&amp;#039;(0)=1$, so define&lt;br /&gt;
$$ \mathcal{F}_0 = \{ f_0 \colon f_0 \quad\text{is defined and analytic in a neighborhood of 0}\quad f_0(0)=0, f_0&amp;#039;(0)=1, f_0&amp;#039;&amp;#039;(0)=1\}$$&lt;br /&gt;
&lt;br /&gt;
== Neighborhood of $f$ in the compact-open topology with domain of definition ==&lt;br /&gt;
&amp;amp;#91; p. 332 &amp;amp;#93;&lt;br /&gt;
&lt;br /&gt;
In what follows a map $f$ is always associated with its domain of definition $D(f)$. That is two maps are considered as distinct if they have distinct domains, even if the one is an extension of the other. A neighborhood of an analytic map $f\colon D(f)\to\overline{\C}$ is a set containing&lt;br /&gt;
$$\{ g \colon g \quad\text{is analytic},\quad D(g)\supset K, \sup_{z\in K} d(f(z)-g(z))&amp;lt;\eps \} $$&lt;br /&gt;
where $K$ is a compact set in $D(f)$, $\eps&amp;gt;0$ and $d(.,.)$ is the spherical metric.&lt;br /&gt;
A sequence $(f_n)$ converges to $f$ in this topology if and only if for any compact set $K\subset D(f)$ there exists $n_0$ such that $K\subset D(f_n)$ for all $n\ge n_0$ and $f_n|_K\to f|_K$ uniformly on $K$ as $n\to\infty$. The system of these neighborhoods define the &amp;quot;compact-open topology together with the domain of defintion&amp;quot;, which is unfortunately not Hausdorff, since an extension of $f$ is contained in any neighborhood of $f$.&lt;br /&gt;
&lt;br /&gt;
For $b_1,b_2\in\C$ with $\Re(b_1)&amp;lt;\Re(b_2)$ define &lt;br /&gt;
$$Q(b_1,b_2)=\{z\in\C\colon \Re(z-b_1)&amp;gt;-|\Im(z-b_1)|, \Re(z-b_2)&amp;gt;|\Im(z-b_2)|\}$$&lt;br /&gt;
If $b_1=-\infty$ (resp. $b_2=\infty$) then the corresponding condition should be removed.&lt;br /&gt;
&lt;br /&gt;
== Proposition 2.5.2 ==&lt;br /&gt;
&amp;amp;#91;p. 333&amp;amp;#93;&lt;br /&gt;
&lt;br /&gt;
Let $f$ be a holomorphic function defined on $Q=Q(b_1,b_2)$ with $\Re(b_2)&amp;gt;\Re(b_1)+2$ (here $b_1$ or $b_2$ may be $-\infty$ or $\infty$). Suppose &lt;br /&gt;
$$|F(z)-(z+1)|&amp;lt;\frac{1}{4},\quad |F&amp;#039;(z)-(z+1)|&amp;lt;\frac{1}{4}\quad \text{for all}\quad z\in Q.$$&lt;br /&gt;
&lt;br /&gt;
Then&lt;br /&gt;
# $F$ is univalent &amp;amp;#91;means injective&amp;amp;#93; on $Q$.&lt;br /&gt;
# Let $z_0\in Q$ be a point such that $\Re(b_1)&amp;lt;\Re(z_0)&amp;lt;\Re(b_2)-\frac{5}{4}$. Denote by $S$ the closed region (a strip) bounded by the two curves $\ell=\{z_0+i y\colon y\in\R\}$ and $F(\ell)$. Then for any $z\in Q$ there exist a unique $n\in \Z$ such that $F^n(z)$ is defined and belongs to $S-F(\ell)$.&lt;br /&gt;
# There exists an univalent function $\Phi\colon Q\to \C$ satisfying $$\Phi(F(z))=\Phi(z)+1$$ whenever both sides are defined. Moreover $\Phi$ is unique up to an addition of a constant.&lt;br /&gt;
# Fix a point $z_0\in Q$. If we normalize $\Phi$ by $\Phi(z_0)=0$ then the correspondence $F\mapsto \Phi$ is continuous with respect to the compact-open topology.&lt;br /&gt;
&lt;br /&gt;
== $\mathcal{F}$, $\mathcal{F}_1$ and $\alpha(f)$ ==&lt;br /&gt;
&amp;amp;#91;p. 339&amp;amp;#93;&lt;br /&gt;
&lt;br /&gt;
$$ \mathcal{F} = \{ f \colon f \quad\text{is defined and analytic in a neighborhood of 0}\quad f(0)=0, f_0&amp;#039;(0)\neq 0\}$$&lt;br /&gt;
For $f\in \mathcal{F}$ we express the derivative &lt;br /&gt;
$$f&amp;#039;(0)=\exp(2\pi i \alpha(f))$$&lt;br /&gt;
where $\alpha(f)\in\C$ and $-\frac{1}{2} &amp;lt; \Re(\alpha(f)) \le \frac{1}{2}$ our study is focussed on the maps in the following class&lt;br /&gt;
$$ \mathcal{F}_1 = \{ f\in \mathcal{F}\colon |\arg(\alpha(f))| &amp;lt; \frac{\pi}{4}\} $$&lt;br /&gt;
&lt;br /&gt;
=== Comments ===&lt;br /&gt;
&lt;br /&gt;
By the definition we have $$&lt;br /&gt;
\begin{align*}&lt;br /&gt;
\log(f&amp;#039;(0))&amp;amp;=2\pi i\alpha(f)=2\pi i re^{i\beta}=2\pi r e^{i(\beta+\frac{\pi}{2})}\\&lt;br /&gt;
\arg(\log(f&amp;#039;(0))&amp;amp;=\beta+\frac{\pi}{2}&lt;br /&gt;
\end{align*}$$&lt;br /&gt;
so the condition for $\mathcal{F}_1$ is&lt;br /&gt;
$|\arg(\log(f&amp;#039;(0)))-\frac{\pi}{2}|&amp;lt;\frac{\pi}{4}$ or&lt;br /&gt;
$$\frac{\pi}{4} &amp;lt; \arg(\log(f&amp;#039;(0)) &amp;lt; \frac{3\pi}{4}$$&lt;br /&gt;
&lt;br /&gt;
== $\sigma(f)$ ==&lt;br /&gt;
&amp;amp;#91;p. 340&amp;amp;#93;&lt;br /&gt;
&lt;br /&gt;
Let $\sigma(f)$ be the other fixpoint of $f$ (besides 0).&lt;br /&gt;
&lt;br /&gt;
...&lt;br /&gt;
&lt;br /&gt;
$$\sigma(f) = 2\pi i \alpha(f)(1+o(1)), \quad\text{as}\quad f\to f_0$$&lt;br /&gt;
&lt;br /&gt;
=== Comments ===&lt;br /&gt;
&lt;br /&gt;
By the comment before, we can say that $\sigma(f)$ lies roughly in the sector of angle $(\frac{\pi}{4},\frac{3\pi}{4})$ above the tip 0.&lt;br /&gt;
&lt;br /&gt;
== Proposition 3.2.2 ==&lt;br /&gt;
[p. 340]&lt;br /&gt;
&lt;br /&gt;
Let $f_0\in\mathcal{F}_0$. There exists a neighborhood $\mathcal{N}_0$ of $f_0$ (in the sense of the topology defined in 2.5.1) such that if $f\in\mathcal{N}_0\cap \mathcal{F}_1$, then there exist closed Jordan domains $S_{-,f}$, $S_{+,f}$ and analytic functions $\Phi_{-,f}$, $\Phi_{+,f}$ satisfying the following:&lt;br /&gt;
&lt;br /&gt;
(i) $S_{+,f}$ is bounded by an arc $\ell_{\pm}$ and its image $f(\ell_{\pm})$ such that $\ell_{\pm}$ joins two fixed points $\{0,\sigma(f)\}$, $\ell_{\pm}\cap f(\ell_{\pm}) = \{0,\sigma(f)\}$ and $S_{-,f}\cap S_{+,f} = \{0,\sigma(f)\}$; &lt;br /&gt;
&lt;br /&gt;
(ii) $\Phi_{\pm,f}$ is defined, analytic and injective in a neighborhood of $S&amp;#039;_{\pm,f} = S_{\pm,f}\setminus \{0,\sigma(f)\}$;&lt;br /&gt;
&lt;br /&gt;
(iii) if $z\in S&amp;#039;_{-,f}$ then there is an $n\ge 1$ such that $f^n(z)\in S&amp;#039;_{+,f}$ and for the smallest such $n$,&lt;br /&gt;
\[ \Phi_{+,f}(f^n(z)) = \Phi_{-,f}(z) - \frac{1}{\alpha(f)} + n \]&lt;br /&gt;
&lt;br /&gt;
(iv) when $f\in\mathcal{F}_1$ tends to $f_0$, $S_{\pm,f}\to S_{\pm,0}\cup \{0\}$ in the Hausdorff metric, and $\Phi_{\pm,f}\to \Phi_{\pm,0}$ in the topology defined in 2.5.1.&lt;br /&gt;
&lt;br /&gt;
== Proposition 4.4.1 ==&lt;br /&gt;
&amp;amp;#91;p. 356&amp;amp;#93;&lt;br /&gt;
&lt;br /&gt;
Let $f_0\in\mathcal{F}_0$, there exists a neighborhood $\mathcal{N}_0$ of $f_0$ (in the previously described &amp;quot;compact-open topology with domain of definition&amp;quot;), such that if $f\in \mathcal{N}_0 \cap \mathcal{F}_1$, then there exist large $\xi_0, \eta_0&amp;gt;0$, and analytic maps $\ph_f\colon D(\ph_f)\to\overline{\C}$ and $\tilde{\mathcal{R}}_f\colon D(\tilde{\mathcal{R}}_f)\to \C$ satisfying the following:&lt;br /&gt;
# $D(\ph_f)$ contains the set $$ \mathcal{Q}_f = \{ w\in\C\colon |\arg(-w-\xi_0)| &amp;lt; \frac{2\pi}{3}, |\arg(w+\frac{1}{\alpha(f)}-\xi_0)|&amp;lt;\frac{2\pi}{3} \} $$ and $\ph_f(D(\ph_f)) \subseteq D(f)$; If $w, w+1\in D(\ph_f)$ then $$ \ph_f(w+1)=f(\ph_f(w)) $$ $\ph_f(w)\to 0$ when $w\in \mathcal{Q}_f$ and $\Im(w)\to\infty$; $\ph_f(w)\to\sigma(f)$ when $w\in\mathcal{Q}_f$ and $\Im(w)\to -\infty$.&lt;br /&gt;
# $D(\tilde{\mathcal{R}}_f)$ contains $\{ w\in\C\colon |\Im(w)| &amp;gt; \eta_0\}$ and is invariant under $T(w)=w+1$; if $w\in D(\tilde{\mathcal{R}}_f)$ then $$\tilde{\mathcal{R}}_f(w+1)=\tilde{\mathcal{R}}(w)+1;$$ $\tilde{\mathcal{R}}_f(w)-w$ tends to $-\frac{1}{\alpha(f)}$ when $\Im(w)\to\infty$; to a constant when $\Im(w)\to -\infty$.&lt;br /&gt;
# If $w\in D(\tilde{\mathcal{R}}_f)\cap D(\ph_f)$ and $w&amp;#039;=\tilde{\mathcal{R}}_f(w)+n\in D(\ph_f)$ for some $n\in\Z$ then $$f^n(\ph_f(w))=\ph_f(w&amp;#039;)\quad \text{for}\quad n\ge 0, \quad f^{-n}(\ph_f(w&amp;#039;))=\ph_f(w)\quad \text{for}\quad n&amp;lt;0$$ Moreover if $|\arg(w&amp;#039;+\frac{1}{2\alpha(f)}-\xi_0)|&amp;lt;\frac{2\pi}{3}$ then $n&amp;gt;0$.&lt;br /&gt;
# When $f\in\mathcal{F_1}$ and $f\to f_0$ $$\ph_f\to\ph_0\quad\text{and}\quad \tilde{\mathcal{R}}_f + \frac{1}{\alpha(f)} \to \tilde{\mathcal{E}}_{f_0}$$&lt;br /&gt;
&lt;br /&gt;
== Proposition A.1 ==&lt;br /&gt;
[p. 360]&lt;br /&gt;
&lt;br /&gt;
In the settings of Proposition 3.2.2 (resp. 2.5.2), assume in addtion that $f_s(z)$ (resp. $F_s(z)$) is a family of holomorphic maps for $s\in \Delta \cup \{0\} \subset \mathbb{C}^k$, with $\Delta\subset\mathbb{C}^k$ an open connected set containing 0 in the boundary, such that $f_s$ (resp. $F_s(z)$) is continuous for $s\in\Delta\cup \{0\}$ and analytic in $s\in\Delta$, then the Fatou coordinates $\Phi_{\pm,f_s}$ (resp. $\Phi_{F_s}$) depend analytically on $s$ for $s\in\Delta$.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;references/&amp;gt;&lt;/div&gt;</summary>
		<author><name>Bo198214</name></author>
	</entry>
	<entry>
		<id>https://tetrationforum.org/hyperops_wiki/index.php?title=Shishikura_perturbed_Fatou_coordinates&amp;diff=154</id>
		<title>Shishikura perturbed Fatou coordinates</title>
		<link rel="alternate" type="text/html" href="https://tetrationforum.org/hyperops_wiki/index.php?title=Shishikura_perturbed_Fatou_coordinates&amp;diff=154"/>
		<updated>2013-02-19T21:49:26Z</updated>

		<summary type="html">&lt;p&gt;Bo198214: /* Proposition A.1 */ fixed typo&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Shishikura writes&amp;lt;ref name=&amp;quot;Shishikura2000&amp;quot;&amp;gt;Shishikura, M. (2000). Bifurcation of parabolic fixed points. In Lei, Tan, The Mandelbrot set, theme and variations. Cambridge: Cambridge University Press. Lond. Math. Soc. Lect. Note Ser. 274, 325-363 (2000)&amp;lt;/ref&amp;gt; the following&lt;br /&gt;
&lt;br /&gt;
== $\mathcal{F}_0$ ==&lt;br /&gt;
&amp;amp;#91;p. 327&amp;amp;#93;&lt;br /&gt;
 &lt;br /&gt;
If $f_0&amp;#039;&amp;#039;(0)\neq 0$ by another coordinate change we may assume that $f_0&amp;#039;&amp;#039;(0)=1$, so define&lt;br /&gt;
$$ \mathcal{F}_0 = \{ f_0 \colon f_0 \quad\text{is defined and analytic in a neighborhood of 0}\quad f_0(0)=0, f_0&amp;#039;(0)=1, f_0&amp;#039;&amp;#039;(0)=1\}$$&lt;br /&gt;
&lt;br /&gt;
== Neighborhood of $f$ in the compact-open topology with domain of definition ==&lt;br /&gt;
&amp;amp;#91; p. 332 &amp;amp;#93;&lt;br /&gt;
&lt;br /&gt;
In what follows a map $f$ is always associated with its domain of definition $D(f)$. That is two maps are considered as distinct if they have distinct domains, even if the one is an extension of the other. A neighborhood of an analytic map $f\colon D(f)\to\overline{\C}$ is a set containing&lt;br /&gt;
$$\{ g \colon g \quad\text{is analytic},\quad D(g)\supset K, \sup_{z\in K} d(f(z)-g(z))&amp;lt;\eps \} $$&lt;br /&gt;
where $K$ is a compact set in $D(f)$, $\eps&amp;gt;0$ and $d(.,.)$ is the spherical metric.&lt;br /&gt;
A sequence $(f_n)$ converges to $f$ in this topology if and only if for any compact set $K\subset D(f)$ there exists $n_0$ such that $K\subset D(f_n)$ for all $n\ge n_0$ and $f_n|_K\to f|_K$ uniformly on $K$ as $n\to\infty$. The system of these neighborhoods define the &amp;quot;compact-open topology together with the domain of defintion&amp;quot;, which is unfortunately not Hausdorff, since an extension of $f$ is contained in any neighborhood of $f$.&lt;br /&gt;
&lt;br /&gt;
For $b_1,b_2\in\C$ with $\Re(b_1)&amp;lt;\Re(b_2)$ define &lt;br /&gt;
$$Q(b_1,b_2)=\{z\in\C\colon \Re(z-b_1)&amp;gt;-|\Im(z-b_1)|, \Re(z-b_2)&amp;gt;|\Im(z-b_2)|\}$$&lt;br /&gt;
If $b_1=-\infty$ (resp. $b_2=\infty$) then the corresponding condition should be removed.&lt;br /&gt;
&lt;br /&gt;
== Proposition 2.5.2 ==&lt;br /&gt;
&amp;amp;#91;p. 333&amp;amp;#93;&lt;br /&gt;
&lt;br /&gt;
Let $f$ be a holomorphic function defined on $Q=Q(b_1,b_2)$ with $\Re(b_2)&amp;gt;\Re(b_1)+2$ (here $b_1$ or $b_2$ may be $-\infty$ or $\infty$). Suppose &lt;br /&gt;
$$|F(z)-(z+1)|&amp;lt;\frac{1}{4},\quad |F&amp;#039;(z)-(z+1)|&amp;lt;\frac{1}{4}\quad \text{for all}\quad z\in Q.$$&lt;br /&gt;
&lt;br /&gt;
Then&lt;br /&gt;
# $F$ is univalent &amp;amp;#91;means injective&amp;amp;#93; on $Q$.&lt;br /&gt;
# Let $z_0\in Q$ be a point such that $\Re(b_1)&amp;lt;\Re(z_0)&amp;lt;\Re(b_2)-\frac{5}{4}$. Denote by $S$ the closed region (a strip) bounded by the two curves $\ell=\{z_0+i y\colon y\in\R\}$ and $F(\ell)$. Then for any $z\in Q$ there exist a unique $n\in \Z$ such that $F^n(z)$ is defined and belongs to $S-F(\ell)$.&lt;br /&gt;
# There exists an univalent function $\Phi\colon Q\to \C$ satisfying $$\Phi(F(z))=\Phi(z)+1$$ whenever both sides are defined. Moreover $\Phi$ is unique up to an addition of a constant.&lt;br /&gt;
# Fix a point $z_0\in Q$. If we normalize $\Phi$ by $\Phi(z_0)=0$ then the correspondence $F\mapsto \Phi$ is continuous with respect to the compact-open topology.&lt;br /&gt;
&lt;br /&gt;
== $\mathcal{F}$, $\mathcal{F}_1$ and $\alpha(f)$ ==&lt;br /&gt;
&amp;amp;#91;p. 339&amp;amp;#93;&lt;br /&gt;
&lt;br /&gt;
$$ \mathcal{F} = \{ f \colon f \quad\text{is defined and analytic in a neighborhood of 0}\quad f(0)=0, f_0&amp;#039;(0)\neq 0\}$$&lt;br /&gt;
For $f\in \mathcal{F}$ we express the derivative &lt;br /&gt;
$$f&amp;#039;(0)=\exp(2\pi i \alpha(f))$$&lt;br /&gt;
where $\alpha(f)\in\C$ and $-\frac{1}{2} &amp;lt; \Re(\alpha(f)) \le \frac{1}{2}$ our study is focussed on the maps in the following class&lt;br /&gt;
$$ \mathcal{F}_1 = \{ f\in \mathcal{F}\colon |\arg(\alpha(f))| &amp;lt; \frac{\pi}{4}\} $$&lt;br /&gt;
&lt;br /&gt;
=== Comments ===&lt;br /&gt;
&lt;br /&gt;
By the definition we have $$&lt;br /&gt;
\begin{align*}&lt;br /&gt;
\log(f&amp;#039;(0))&amp;amp;=2\pi i\alpha(f)=2\pi i re^{i\beta}=2\pi r e^{i(\beta+\frac{\pi}{2})}\\&lt;br /&gt;
\arg(\log(f&amp;#039;(0))&amp;amp;=\beta+\frac{\pi}{2}&lt;br /&gt;
\end{align*}$$&lt;br /&gt;
so the condition for $\mathcal{F}_1$ is&lt;br /&gt;
$|\arg(\log(f&amp;#039;(0)))-\frac{\pi}{2}|&amp;lt;\frac{\pi}{4}$ or&lt;br /&gt;
$$\frac{\pi}{4} &amp;lt; \arg(\log(f&amp;#039;(0)) &amp;lt; \frac{3\pi}{4}$$&lt;br /&gt;
&lt;br /&gt;
== $\sigma(f)$ ==&lt;br /&gt;
&amp;amp;#91;p. 340&amp;amp;#93;&lt;br /&gt;
&lt;br /&gt;
Let $\sigma(f)$ be the other fixpoint of $f$ (besides 0).&lt;br /&gt;
&lt;br /&gt;
...&lt;br /&gt;
&lt;br /&gt;
$$\sigma(f) = 2\pi i \alpha(f)(1+o(1)), \quad\text{as}\quad f\to f_0$$&lt;br /&gt;
&lt;br /&gt;
=== Comments ===&lt;br /&gt;
&lt;br /&gt;
By the comment before, we can say that $\sigma(f)$ lies roughly in the sector of angle $(\frac{\pi}{4},\frac{3\pi}{4})$ above the tip 0.&lt;br /&gt;
&lt;br /&gt;
== Proposition 3.2.2 ==&lt;br /&gt;
[p. 340]&lt;br /&gt;
&lt;br /&gt;
Let $f_0\in\mathcal{F}_0$. There exists a neighborhood $\mathcal{N}_0$ of $f_0$ (in the sense of the topology defined in 2.5.1) such that if $f\in\mathcal{N}_0\cap \mathcal{F}_1$, then there exist closed Jordan domains $S_{-,f}$, $S_{+,f}$ and analytic functions $\Phi_{-,f}$, $\Phi_{+,f}$ satisfying the following:&lt;br /&gt;
&lt;br /&gt;
(i) $S_{+,f}$ is bounded by an arc $\ell_{\pm}$ and its image $f(\ell_{\pm})$ such that $\ell_{\pm}$ joins two fixed points $\{0,\sigma(f)\}$, $\ell_{\pm}\cap f(\ell_{\pm}) = \{0,\sigma(f)\}$ and $S_{-,f}\cap S_{+,f} = \{0,\sigma(f)\}$; &lt;br /&gt;
&lt;br /&gt;
(ii) $\Phi_{\pm,f}$ is defined, analytic and injective in a neighborhood of $S&amp;#039;_{\pm,f} = S_{\pm,f}\setminus \{0,\sigma(f)\}$;&lt;br /&gt;
&lt;br /&gt;
(iii) if $z\in S&amp;#039;_{-,f}$ then there is an $n\ge 1$ such that $f^n(z)\in S&amp;#039;_{+,f}$ and for the smallest such $n$,&lt;br /&gt;
\[ \Phi_{+,f}(f^n(z)) = \Phi_{-,f}(z) - \frac{1}{\alpha(f)} + n \]&lt;br /&gt;
&lt;br /&gt;
(iv) when $f\in\mathcal{F}_1$ tends to $f_0$, $S_{\pm,f}\to S_{\pm,0}\cup \{0\}$ in the Hausdorff metric, and $\Phi_{\pm,f}\to \Phi_{\pm,0}$ in the topology defined in 2.5.1.&lt;br /&gt;
&lt;br /&gt;
== Proposition 4.4.1 ==&lt;br /&gt;
&amp;amp;#91;p. 356&amp;amp;#93;&lt;br /&gt;
&lt;br /&gt;
Let $f_0\in\mathcal{F}_0$, there exists a neighborhood $\mathcal{N}_0$ of $f_0$ (in the previously described &amp;quot;compact-open topology with domain of definition&amp;quot;), such that if $f\in \mathcal{N}_0 \cap \mathcal{F}_1$, then there exist large $\xi_0, \eta_0&amp;gt;0$, and analytic maps $\ph_f\colon D(\ph_f)\to\overline{\C}$ and $\tilde{\mathcal{R}}_f\colon D(\tilde{\mathcal{R}}_f)\to \C$ satisfying the following:&lt;br /&gt;
# $D(\ph_f)$ contains the set $$ \mathcal{Q}_f = \{ w\in\C\colon |\arg(-w-\xi_0)| &amp;lt; \frac{2\pi}{3}, |\arg(w+\frac{1}{\alpha(f)}-\xi_0)|&amp;lt;\frac{2\pi}{3} \} $$ and $\ph_f(D(\ph_f)) \subseteq D(f)$; If $w, w+1\in D(\ph_f)$ then $$ \ph_f(w+1)=f(\ph_f(w)) $$ $\ph_f(w)\to 0$ when $w\in \mathcal{Q}_f$ and $\Im(w)\to\infty$; $\ph_f(w)\to\sigma(f)$ when $w\in\mathcal{Q}_f$ and $\Im(w)\to -\infty$.&lt;br /&gt;
# $D(\tilde{\mathcal{R}}_f)$ contains $\{ w\in\C\colon |\Im(w)| &amp;gt; \eta_0\}$ and is invariant under $T(w)=w+1$; if $w\in D(\tilde{\mathcal{R}}_f)$ then $$\tilde{\mathcal{R}}_f(w+1)=\tilde{\mathcal{R}}(w)+1;$$ $\tilde{\mathcal{R}}_f(w)-w$ tends to $-\frac{1}{\alpha(f)}$ when $\Im(w)\to\infty$; to a constant when $\Im(w)\to -\infty$.&lt;br /&gt;
# If $w\in D(\tilde{\mathcal{R}}_f)\cap D(\ph_f)$ and $w&amp;#039;=\tilde{\mathcal{R}}_f(w)+n\in D(\ph_f)$ for some $n\in\Z$ then $$f^n(\ph_f(w))=\ph_f(w&amp;#039;)\quad \text{for}\quad n\ge 0, \quad f^{-n}(\ph_f(w&amp;#039;))=\ph_f(w)\quad \text{for}\quad n&amp;lt;0$$ Moreover if $|\arg(w&amp;#039;+\frac{1}{2\alpha(f)}-\xi_0)|&amp;lt;\frac{2\pi}{3}$ then $n&amp;gt;0$.&lt;br /&gt;
# When $f\in\mathcal{F_1}$ and $f\to f_0$ $$\ph_f\to\ph_0\quad\text{and}\quad \tilde{\mathcal{R}}_f + \frac{1}{\alpha(f)} \to \tilde{\mathcal{E}}_{f_0}$$&lt;br /&gt;
&lt;br /&gt;
== Proposition A.1 ==&lt;br /&gt;
In the settings of Proposition 3.2.2 (resp. 2.5.2), assume in addtion that $f_s(z)$ (resp. $F_s(z)$) is a family of holomorphic maps for $s\in \Delta \cup \{0\} \subset \mathbb{C}^k$, with $\Delta\subset\mathbb{C}^k$ an open connected set containing 0 in the boundary, such that $f_s$ (resp. $F_s(z)$) is continuous for $s\in\Delta\cup \{0\}$ and analytic in $s\in\Delta$, then the Fatou coordinates $\Phi_{\pm,f_s}$ (resp. $\Phi_{F_s}$) depend analytically on $s$ for $s\in\Delta$.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;references/&amp;gt;&lt;/div&gt;</summary>
		<author><name>Bo198214</name></author>
	</entry>
	<entry>
		<id>https://tetrationforum.org/hyperops_wiki/index.php?title=Shishikura_perturbed_Fatou_coordinates&amp;diff=153</id>
		<title>Shishikura perturbed Fatou coordinates</title>
		<link rel="alternate" type="text/html" href="https://tetrationforum.org/hyperops_wiki/index.php?title=Shishikura_perturbed_Fatou_coordinates&amp;diff=153"/>
		<updated>2013-02-19T21:48:47Z</updated>

		<summary type="html">&lt;p&gt;Bo198214: /* Proposition A.1 */ removed unnecessary notation&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Shishikura writes&amp;lt;ref name=&amp;quot;Shishikura2000&amp;quot;&amp;gt;Shishikura, M. (2000). Bifurcation of parabolic fixed points. In Lei, Tan, The Mandelbrot set, theme and variations. Cambridge: Cambridge University Press. Lond. Math. Soc. Lect. Note Ser. 274, 325-363 (2000)&amp;lt;/ref&amp;gt; the following&lt;br /&gt;
&lt;br /&gt;
== $\mathcal{F}_0$ ==&lt;br /&gt;
&amp;amp;#91;p. 327&amp;amp;#93;&lt;br /&gt;
 &lt;br /&gt;
If $f_0&amp;#039;&amp;#039;(0)\neq 0$ by another coordinate change we may assume that $f_0&amp;#039;&amp;#039;(0)=1$, so define&lt;br /&gt;
$$ \mathcal{F}_0 = \{ f_0 \colon f_0 \quad\text{is defined and analytic in a neighborhood of 0}\quad f_0(0)=0, f_0&amp;#039;(0)=1, f_0&amp;#039;&amp;#039;(0)=1\}$$&lt;br /&gt;
&lt;br /&gt;
== Neighborhood of $f$ in the compact-open topology with domain of definition ==&lt;br /&gt;
&amp;amp;#91; p. 332 &amp;amp;#93;&lt;br /&gt;
&lt;br /&gt;
In what follows a map $f$ is always associated with its domain of definition $D(f)$. That is two maps are considered as distinct if they have distinct domains, even if the one is an extension of the other. A neighborhood of an analytic map $f\colon D(f)\to\overline{\C}$ is a set containing&lt;br /&gt;
$$\{ g \colon g \quad\text{is analytic},\quad D(g)\supset K, \sup_{z\in K} d(f(z)-g(z))&amp;lt;\eps \} $$&lt;br /&gt;
where $K$ is a compact set in $D(f)$, $\eps&amp;gt;0$ and $d(.,.)$ is the spherical metric.&lt;br /&gt;
A sequence $(f_n)$ converges to $f$ in this topology if and only if for any compact set $K\subset D(f)$ there exists $n_0$ such that $K\subset D(f_n)$ for all $n\ge n_0$ and $f_n|_K\to f|_K$ uniformly on $K$ as $n\to\infty$. The system of these neighborhoods define the &amp;quot;compact-open topology together with the domain of defintion&amp;quot;, which is unfortunately not Hausdorff, since an extension of $f$ is contained in any neighborhood of $f$.&lt;br /&gt;
&lt;br /&gt;
For $b_1,b_2\in\C$ with $\Re(b_1)&amp;lt;\Re(b_2)$ define &lt;br /&gt;
$$Q(b_1,b_2)=\{z\in\C\colon \Re(z-b_1)&amp;gt;-|\Im(z-b_1)|, \Re(z-b_2)&amp;gt;|\Im(z-b_2)|\}$$&lt;br /&gt;
If $b_1=-\infty$ (resp. $b_2=\infty$) then the corresponding condition should be removed.&lt;br /&gt;
&lt;br /&gt;
== Proposition 2.5.2 ==&lt;br /&gt;
&amp;amp;#91;p. 333&amp;amp;#93;&lt;br /&gt;
&lt;br /&gt;
Let $f$ be a holomorphic function defined on $Q=Q(b_1,b_2)$ with $\Re(b_2)&amp;gt;\Re(b_1)+2$ (here $b_1$ or $b_2$ may be $-\infty$ or $\infty$). Suppose &lt;br /&gt;
$$|F(z)-(z+1)|&amp;lt;\frac{1}{4},\quad |F&amp;#039;(z)-(z+1)|&amp;lt;\frac{1}{4}\quad \text{for all}\quad z\in Q.$$&lt;br /&gt;
&lt;br /&gt;
Then&lt;br /&gt;
# $F$ is univalent &amp;amp;#91;means injective&amp;amp;#93; on $Q$.&lt;br /&gt;
# Let $z_0\in Q$ be a point such that $\Re(b_1)&amp;lt;\Re(z_0)&amp;lt;\Re(b_2)-\frac{5}{4}$. Denote by $S$ the closed region (a strip) bounded by the two curves $\ell=\{z_0+i y\colon y\in\R\}$ and $F(\ell)$. Then for any $z\in Q$ there exist a unique $n\in \Z$ such that $F^n(z)$ is defined and belongs to $S-F(\ell)$.&lt;br /&gt;
# There exists an univalent function $\Phi\colon Q\to \C$ satisfying $$\Phi(F(z))=\Phi(z)+1$$ whenever both sides are defined. Moreover $\Phi$ is unique up to an addition of a constant.&lt;br /&gt;
# Fix a point $z_0\in Q$. If we normalize $\Phi$ by $\Phi(z_0)=0$ then the correspondence $F\mapsto \Phi$ is continuous with respect to the compact-open topology.&lt;br /&gt;
&lt;br /&gt;
== $\mathcal{F}$, $\mathcal{F}_1$ and $\alpha(f)$ ==&lt;br /&gt;
&amp;amp;#91;p. 339&amp;amp;#93;&lt;br /&gt;
&lt;br /&gt;
$$ \mathcal{F} = \{ f \colon f \quad\text{is defined and analytic in a neighborhood of 0}\quad f(0)=0, f_0&amp;#039;(0)\neq 0\}$$&lt;br /&gt;
For $f\in \mathcal{F}$ we express the derivative &lt;br /&gt;
$$f&amp;#039;(0)=\exp(2\pi i \alpha(f))$$&lt;br /&gt;
where $\alpha(f)\in\C$ and $-\frac{1}{2} &amp;lt; \Re(\alpha(f)) \le \frac{1}{2}$ our study is focussed on the maps in the following class&lt;br /&gt;
$$ \mathcal{F}_1 = \{ f\in \mathcal{F}\colon |\arg(\alpha(f))| &amp;lt; \frac{\pi}{4}\} $$&lt;br /&gt;
&lt;br /&gt;
=== Comments ===&lt;br /&gt;
&lt;br /&gt;
By the definition we have $$&lt;br /&gt;
\begin{align*}&lt;br /&gt;
\log(f&amp;#039;(0))&amp;amp;=2\pi i\alpha(f)=2\pi i re^{i\beta}=2\pi r e^{i(\beta+\frac{\pi}{2})}\\&lt;br /&gt;
\arg(\log(f&amp;#039;(0))&amp;amp;=\beta+\frac{\pi}{2}&lt;br /&gt;
\end{align*}$$&lt;br /&gt;
so the condition for $\mathcal{F}_1$ is&lt;br /&gt;
$|\arg(\log(f&amp;#039;(0)))-\frac{\pi}{2}|&amp;lt;\frac{\pi}{4}$ or&lt;br /&gt;
$$\frac{\pi}{4} &amp;lt; \arg(\log(f&amp;#039;(0)) &amp;lt; \frac{3\pi}{4}$$&lt;br /&gt;
&lt;br /&gt;
== $\sigma(f)$ ==&lt;br /&gt;
&amp;amp;#91;p. 340&amp;amp;#93;&lt;br /&gt;
&lt;br /&gt;
Let $\sigma(f)$ be the other fixpoint of $f$ (besides 0).&lt;br /&gt;
&lt;br /&gt;
...&lt;br /&gt;
&lt;br /&gt;
$$\sigma(f) = 2\pi i \alpha(f)(1+o(1)), \quad\text{as}\quad f\to f_0$$&lt;br /&gt;
&lt;br /&gt;
=== Comments ===&lt;br /&gt;
&lt;br /&gt;
By the comment before, we can say that $\sigma(f)$ lies roughly in the sector of angle $(\frac{\pi}{4},\frac{3\pi}{4})$ above the tip 0.&lt;br /&gt;
&lt;br /&gt;
== Proposition 3.2.2 ==&lt;br /&gt;
[p. 340]&lt;br /&gt;
&lt;br /&gt;
Let $f_0\in\mathcal{F}_0$. There exists a neighborhood $\mathcal{N}_0$ of $f_0$ (in the sense of the topology defined in 2.5.1) such that if $f\in\mathcal{N}_0\cap \mathcal{F}_1$, then there exist closed Jordan domains $S_{-,f}$, $S_{+,f}$ and analytic functions $\Phi_{-,f}$, $\Phi_{+,f}$ satisfying the following:&lt;br /&gt;
&lt;br /&gt;
(i) $S_{+,f}$ is bounded by an arc $\ell_{\pm}$ and its image $f(\ell_{\pm})$ such that $\ell_{\pm}$ joins two fixed points $\{0,\sigma(f)\}$, $\ell_{\pm}\cap f(\ell_{\pm}) = \{0,\sigma(f)\}$ and $S_{-,f}\cap S_{+,f} = \{0,\sigma(f)\}$; &lt;br /&gt;
&lt;br /&gt;
(ii) $\Phi_{\pm,f}$ is defined, analytic and injective in a neighborhood of $S&amp;#039;_{\pm,f} = S_{\pm,f}\setminus \{0,\sigma(f)\}$;&lt;br /&gt;
&lt;br /&gt;
(iii) if $z\in S&amp;#039;_{-,f}$ then there is an $n\ge 1$ such that $f^n(z)\in S&amp;#039;_{+,f}$ and for the smallest such $n$,&lt;br /&gt;
\[ \Phi_{+,f}(f^n(z)) = \Phi_{-,f}(z) - \frac{1}{\alpha(f)} + n \]&lt;br /&gt;
&lt;br /&gt;
(iv) when $f\in\mathcal{F}_1$ tends to $f_0$, $S_{\pm,f}\to S_{\pm,0}\cup \{0\}$ in the Hausdorff metric, and $\Phi_{\pm,f}\to \Phi_{\pm,0}$ in the topology defined in 2.5.1.&lt;br /&gt;
&lt;br /&gt;
== Proposition 4.4.1 ==&lt;br /&gt;
&amp;amp;#91;p. 356&amp;amp;#93;&lt;br /&gt;
&lt;br /&gt;
Let $f_0\in\mathcal{F}_0$, there exists a neighborhood $\mathcal{N}_0$ of $f_0$ (in the previously described &amp;quot;compact-open topology with domain of definition&amp;quot;), such that if $f\in \mathcal{N}_0 \cap \mathcal{F}_1$, then there exist large $\xi_0, \eta_0&amp;gt;0$, and analytic maps $\ph_f\colon D(\ph_f)\to\overline{\C}$ and $\tilde{\mathcal{R}}_f\colon D(\tilde{\mathcal{R}}_f)\to \C$ satisfying the following:&lt;br /&gt;
# $D(\ph_f)$ contains the set $$ \mathcal{Q}_f = \{ w\in\C\colon |\arg(-w-\xi_0)| &amp;lt; \frac{2\pi}{3}, |\arg(w+\frac{1}{\alpha(f)}-\xi_0)|&amp;lt;\frac{2\pi}{3} \} $$ and $\ph_f(D(\ph_f)) \subseteq D(f)$; If $w, w+1\in D(\ph_f)$ then $$ \ph_f(w+1)=f(\ph_f(w)) $$ $\ph_f(w)\to 0$ when $w\in \mathcal{Q}_f$ and $\Im(w)\to\infty$; $\ph_f(w)\to\sigma(f)$ when $w\in\mathcal{Q}_f$ and $\Im(w)\to -\infty$.&lt;br /&gt;
# $D(\tilde{\mathcal{R}}_f)$ contains $\{ w\in\C\colon |\Im(w)| &amp;gt; \eta_0\}$ and is invariant under $T(w)=w+1$; if $w\in D(\tilde{\mathcal{R}}_f)$ then $$\tilde{\mathcal{R}}_f(w+1)=\tilde{\mathcal{R}}(w)+1;$$ $\tilde{\mathcal{R}}_f(w)-w$ tends to $-\frac{1}{\alpha(f)}$ when $\Im(w)\to\infty$; to a constant when $\Im(w)\to -\infty$.&lt;br /&gt;
# If $w\in D(\tilde{\mathcal{R}}_f)\cap D(\ph_f)$ and $w&amp;#039;=\tilde{\mathcal{R}}_f(w)+n\in D(\ph_f)$ for some $n\in\Z$ then $$f^n(\ph_f(w))=\ph_f(w&amp;#039;)\quad \text{for}\quad n\ge 0, \quad f^{-n}(\ph_f(w&amp;#039;))=\ph_f(w)\quad \text{for}\quad n&amp;lt;0$$ Moreover if $|\arg(w&amp;#039;+\frac{1}{2\alpha(f)}-\xi_0)|&amp;lt;\frac{2\pi}{3}$ then $n&amp;gt;0$.&lt;br /&gt;
# When $f\in\mathcal{F_1}$ and $f\to f_0$ $$\ph_f\to\ph_0\quad\text{and}\quad \tilde{\mathcal{R}}_f + \frac{1}{\alpha(f)} \to \tilde{\mathcal{E}}_{f_0}$$&lt;br /&gt;
&lt;br /&gt;
== Proposition A.1 ==&lt;br /&gt;
In the settings of Proposition 3.2.2 (resp. 2.5.2), assume in addtion that $f_s(z)$ (resp. $F_s(z)$) is a family of holomorphic maps for $s\in \Delta \cup \{0\} \subset \mathbb{C}^k$, with $\Delta\subset\mathbb{C}^k$ an open connected set containing 0 in the boundary, such that $f_s$ (resp. $F_s(z)$) is continuous for $s\in\Delta\cup \{0\}$ and analytic in $s\in\Delta$, the the Fatou coordinates $\Phi_{\pm,f_s}$ (resp. $\Phi_{F_s}$) depend analytically on $s$ for $s\in\Delta$.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;references/&amp;gt;&lt;/div&gt;</summary>
		<author><name>Bo198214</name></author>
	</entry>
	<entry>
		<id>https://tetrationforum.org/hyperops_wiki/index.php?title=Shishikura_perturbed_Fatou_coordinates&amp;diff=152</id>
		<title>Shishikura perturbed Fatou coordinates</title>
		<link rel="alternate" type="text/html" href="https://tetrationforum.org/hyperops_wiki/index.php?title=Shishikura_perturbed_Fatou_coordinates&amp;diff=152"/>
		<updated>2013-02-19T21:46:58Z</updated>

		<summary type="html">&lt;p&gt;Bo198214: /* Proposition A.1 */ wrote Proposition A.1&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Shishikura writes&amp;lt;ref name=&amp;quot;Shishikura2000&amp;quot;&amp;gt;Shishikura, M. (2000). Bifurcation of parabolic fixed points. In Lei, Tan, The Mandelbrot set, theme and variations. Cambridge: Cambridge University Press. Lond. Math. Soc. Lect. Note Ser. 274, 325-363 (2000)&amp;lt;/ref&amp;gt; the following&lt;br /&gt;
&lt;br /&gt;
== $\mathcal{F}_0$ ==&lt;br /&gt;
&amp;amp;#91;p. 327&amp;amp;#93;&lt;br /&gt;
 &lt;br /&gt;
If $f_0&amp;#039;&amp;#039;(0)\neq 0$ by another coordinate change we may assume that $f_0&amp;#039;&amp;#039;(0)=1$, so define&lt;br /&gt;
$$ \mathcal{F}_0 = \{ f_0 \colon f_0 \quad\text{is defined and analytic in a neighborhood of 0}\quad f_0(0)=0, f_0&amp;#039;(0)=1, f_0&amp;#039;&amp;#039;(0)=1\}$$&lt;br /&gt;
&lt;br /&gt;
== Neighborhood of $f$ in the compact-open topology with domain of definition ==&lt;br /&gt;
&amp;amp;#91; p. 332 &amp;amp;#93;&lt;br /&gt;
&lt;br /&gt;
In what follows a map $f$ is always associated with its domain of definition $D(f)$. That is two maps are considered as distinct if they have distinct domains, even if the one is an extension of the other. A neighborhood of an analytic map $f\colon D(f)\to\overline{\C}$ is a set containing&lt;br /&gt;
$$\{ g \colon g \quad\text{is analytic},\quad D(g)\supset K, \sup_{z\in K} d(f(z)-g(z))&amp;lt;\eps \} $$&lt;br /&gt;
where $K$ is a compact set in $D(f)$, $\eps&amp;gt;0$ and $d(.,.)$ is the spherical metric.&lt;br /&gt;
A sequence $(f_n)$ converges to $f$ in this topology if and only if for any compact set $K\subset D(f)$ there exists $n_0$ such that $K\subset D(f_n)$ for all $n\ge n_0$ and $f_n|_K\to f|_K$ uniformly on $K$ as $n\to\infty$. The system of these neighborhoods define the &amp;quot;compact-open topology together with the domain of defintion&amp;quot;, which is unfortunately not Hausdorff, since an extension of $f$ is contained in any neighborhood of $f$.&lt;br /&gt;
&lt;br /&gt;
For $b_1,b_2\in\C$ with $\Re(b_1)&amp;lt;\Re(b_2)$ define &lt;br /&gt;
$$Q(b_1,b_2)=\{z\in\C\colon \Re(z-b_1)&amp;gt;-|\Im(z-b_1)|, \Re(z-b_2)&amp;gt;|\Im(z-b_2)|\}$$&lt;br /&gt;
If $b_1=-\infty$ (resp. $b_2=\infty$) then the corresponding condition should be removed.&lt;br /&gt;
&lt;br /&gt;
== Proposition 2.5.2 ==&lt;br /&gt;
&amp;amp;#91;p. 333&amp;amp;#93;&lt;br /&gt;
&lt;br /&gt;
Let $f$ be a holomorphic function defined on $Q=Q(b_1,b_2)$ with $\Re(b_2)&amp;gt;\Re(b_1)+2$ (here $b_1$ or $b_2$ may be $-\infty$ or $\infty$). Suppose &lt;br /&gt;
$$|F(z)-(z+1)|&amp;lt;\frac{1}{4},\quad |F&amp;#039;(z)-(z+1)|&amp;lt;\frac{1}{4}\quad \text{for all}\quad z\in Q.$$&lt;br /&gt;
&lt;br /&gt;
Then&lt;br /&gt;
# $F$ is univalent &amp;amp;#91;means injective&amp;amp;#93; on $Q$.&lt;br /&gt;
# Let $z_0\in Q$ be a point such that $\Re(b_1)&amp;lt;\Re(z_0)&amp;lt;\Re(b_2)-\frac{5}{4}$. Denote by $S$ the closed region (a strip) bounded by the two curves $\ell=\{z_0+i y\colon y\in\R\}$ and $F(\ell)$. Then for any $z\in Q$ there exist a unique $n\in \Z$ such that $F^n(z)$ is defined and belongs to $S-F(\ell)$.&lt;br /&gt;
# There exists an univalent function $\Phi\colon Q\to \C$ satisfying $$\Phi(F(z))=\Phi(z)+1$$ whenever both sides are defined. Moreover $\Phi$ is unique up to an addition of a constant.&lt;br /&gt;
# Fix a point $z_0\in Q$. If we normalize $\Phi$ by $\Phi(z_0)=0$ then the correspondence $F\mapsto \Phi$ is continuous with respect to the compact-open topology.&lt;br /&gt;
&lt;br /&gt;
== $\mathcal{F}$, $\mathcal{F}_1$ and $\alpha(f)$ ==&lt;br /&gt;
&amp;amp;#91;p. 339&amp;amp;#93;&lt;br /&gt;
&lt;br /&gt;
$$ \mathcal{F} = \{ f \colon f \quad\text{is defined and analytic in a neighborhood of 0}\quad f(0)=0, f_0&amp;#039;(0)\neq 0\}$$&lt;br /&gt;
For $f\in \mathcal{F}$ we express the derivative &lt;br /&gt;
$$f&amp;#039;(0)=\exp(2\pi i \alpha(f))$$&lt;br /&gt;
where $\alpha(f)\in\C$ and $-\frac{1}{2} &amp;lt; \Re(\alpha(f)) \le \frac{1}{2}$ our study is focussed on the maps in the following class&lt;br /&gt;
$$ \mathcal{F}_1 = \{ f\in \mathcal{F}\colon |\arg(\alpha(f))| &amp;lt; \frac{\pi}{4}\} $$&lt;br /&gt;
&lt;br /&gt;
=== Comments ===&lt;br /&gt;
&lt;br /&gt;
By the definition we have $$&lt;br /&gt;
\begin{align*}&lt;br /&gt;
\log(f&amp;#039;(0))&amp;amp;=2\pi i\alpha(f)=2\pi i re^{i\beta}=2\pi r e^{i(\beta+\frac{\pi}{2})}\\&lt;br /&gt;
\arg(\log(f&amp;#039;(0))&amp;amp;=\beta+\frac{\pi}{2}&lt;br /&gt;
\end{align*}$$&lt;br /&gt;
so the condition for $\mathcal{F}_1$ is&lt;br /&gt;
$|\arg(\log(f&amp;#039;(0)))-\frac{\pi}{2}|&amp;lt;\frac{\pi}{4}$ or&lt;br /&gt;
$$\frac{\pi}{4} &amp;lt; \arg(\log(f&amp;#039;(0)) &amp;lt; \frac{3\pi}{4}$$&lt;br /&gt;
&lt;br /&gt;
== $\sigma(f)$ ==&lt;br /&gt;
&amp;amp;#91;p. 340&amp;amp;#93;&lt;br /&gt;
&lt;br /&gt;
Let $\sigma(f)$ be the other fixpoint of $f$ (besides 0).&lt;br /&gt;
&lt;br /&gt;
...&lt;br /&gt;
&lt;br /&gt;
$$\sigma(f) = 2\pi i \alpha(f)(1+o(1)), \quad\text{as}\quad f\to f_0$$&lt;br /&gt;
&lt;br /&gt;
=== Comments ===&lt;br /&gt;
&lt;br /&gt;
By the comment before, we can say that $\sigma(f)$ lies roughly in the sector of angle $(\frac{\pi}{4},\frac{3\pi}{4})$ above the tip 0.&lt;br /&gt;
&lt;br /&gt;
== Proposition 3.2.2 ==&lt;br /&gt;
[p. 340]&lt;br /&gt;
&lt;br /&gt;
Let $f_0\in\mathcal{F}_0$. There exists a neighborhood $\mathcal{N}_0$ of $f_0$ (in the sense of the topology defined in 2.5.1) such that if $f\in\mathcal{N}_0\cap \mathcal{F}_1$, then there exist closed Jordan domains $S_{-,f}$, $S_{+,f}$ and analytic functions $\Phi_{-,f}$, $\Phi_{+,f}$ satisfying the following:&lt;br /&gt;
&lt;br /&gt;
(i) $S_{+,f}$ is bounded by an arc $\ell_{\pm}$ and its image $f(\ell_{\pm})$ such that $\ell_{\pm}$ joins two fixed points $\{0,\sigma(f)\}$, $\ell_{\pm}\cap f(\ell_{\pm}) = \{0,\sigma(f)\}$ and $S_{-,f}\cap S_{+,f} = \{0,\sigma(f)\}$; &lt;br /&gt;
&lt;br /&gt;
(ii) $\Phi_{\pm,f}$ is defined, analytic and injective in a neighborhood of $S&amp;#039;_{\pm,f} = S_{\pm,f}\setminus \{0,\sigma(f)\}$;&lt;br /&gt;
&lt;br /&gt;
(iii) if $z\in S&amp;#039;_{-,f}$ then there is an $n\ge 1$ such that $f^n(z)\in S&amp;#039;_{+,f}$ and for the smallest such $n$,&lt;br /&gt;
\[ \Phi_{+,f}(f^n(z)) = \Phi_{-,f}(z) - \frac{1}{\alpha(f)} + n \]&lt;br /&gt;
&lt;br /&gt;
(iv) when $f\in\mathcal{F}_1$ tends to $f_0$, $S_{\pm,f}\to S_{\pm,0}\cup \{0\}$ in the Hausdorff metric, and $\Phi_{\pm,f}\to \Phi_{\pm,0}$ in the topology defined in 2.5.1.&lt;br /&gt;
&lt;br /&gt;
== Proposition 4.4.1 ==&lt;br /&gt;
&amp;amp;#91;p. 356&amp;amp;#93;&lt;br /&gt;
&lt;br /&gt;
Let $f_0\in\mathcal{F}_0$, there exists a neighborhood $\mathcal{N}_0$ of $f_0$ (in the previously described &amp;quot;compact-open topology with domain of definition&amp;quot;), such that if $f\in \mathcal{N}_0 \cap \mathcal{F}_1$, then there exist large $\xi_0, \eta_0&amp;gt;0$, and analytic maps $\ph_f\colon D(\ph_f)\to\overline{\C}$ and $\tilde{\mathcal{R}}_f\colon D(\tilde{\mathcal{R}}_f)\to \C$ satisfying the following:&lt;br /&gt;
# $D(\ph_f)$ contains the set $$ \mathcal{Q}_f = \{ w\in\C\colon |\arg(-w-\xi_0)| &amp;lt; \frac{2\pi}{3}, |\arg(w+\frac{1}{\alpha(f)}-\xi_0)|&amp;lt;\frac{2\pi}{3} \} $$ and $\ph_f(D(\ph_f)) \subseteq D(f)$; If $w, w+1\in D(\ph_f)$ then $$ \ph_f(w+1)=f(\ph_f(w)) $$ $\ph_f(w)\to 0$ when $w\in \mathcal{Q}_f$ and $\Im(w)\to\infty$; $\ph_f(w)\to\sigma(f)$ when $w\in\mathcal{Q}_f$ and $\Im(w)\to -\infty$.&lt;br /&gt;
# $D(\tilde{\mathcal{R}}_f)$ contains $\{ w\in\C\colon |\Im(w)| &amp;gt; \eta_0\}$ and is invariant under $T(w)=w+1$; if $w\in D(\tilde{\mathcal{R}}_f)$ then $$\tilde{\mathcal{R}}_f(w+1)=\tilde{\mathcal{R}}(w)+1;$$ $\tilde{\mathcal{R}}_f(w)-w$ tends to $-\frac{1}{\alpha(f)}$ when $\Im(w)\to\infty$; to a constant when $\Im(w)\to -\infty$.&lt;br /&gt;
# If $w\in D(\tilde{\mathcal{R}}_f)\cap D(\ph_f)$ and $w&amp;#039;=\tilde{\mathcal{R}}_f(w)+n\in D(\ph_f)$ for some $n\in\Z$ then $$f^n(\ph_f(w))=\ph_f(w&amp;#039;)\quad \text{for}\quad n\ge 0, \quad f^{-n}(\ph_f(w&amp;#039;))=\ph_f(w)\quad \text{for}\quad n&amp;lt;0$$ Moreover if $|\arg(w&amp;#039;+\frac{1}{2\alpha(f)}-\xi_0)|&amp;lt;\frac{2\pi}{3}$ then $n&amp;gt;0$.&lt;br /&gt;
# When $f\in\mathcal{F_1}$ and $f\to f_0$ $$\ph_f\to\ph_0\quad\text{and}\quad \tilde{\mathcal{R}}_f + \frac{1}{\alpha(f)} \to \tilde{\mathcal{E}}_{f_0}$$&lt;br /&gt;
&lt;br /&gt;
== Proposition A.1 ==&lt;br /&gt;
In the settings of Proposition 3.2.2 (resp. 2.5.2), assume in addtion that $f_s(z)$ (resp. $F_s(z)$) is a family of holomorphic maps for $s\in \Delta \cup \{0\} \subset \mathbb{C}^k$, with $\Delta\subset\mathbb{C}^k$ an open connected set containing 0 in the boundary, such that $f_s$ (resp. $F_s(z)$) is continuous for $s\in\Delta\cup \{0\}$ and analytic in $s\in\Delta$, the the Fatou coordinates $\Phi_{\pm,f_s} := \Phi_{\pm,s}$ (resp. $\Phi_s := \Phi_{F_s}$) depend analytically on $s$ for $s\in\Delta$.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;references/&amp;gt;&lt;/div&gt;</summary>
		<author><name>Bo198214</name></author>
	</entry>
	<entry>
		<id>https://tetrationforum.org/hyperops_wiki/index.php?title=Shishikura_perturbed_Fatou_coordinates&amp;diff=151</id>
		<title>Shishikura perturbed Fatou coordinates</title>
		<link rel="alternate" type="text/html" href="https://tetrationforum.org/hyperops_wiki/index.php?title=Shishikura_perturbed_Fatou_coordinates&amp;diff=151"/>
		<updated>2013-02-19T21:40:18Z</updated>

		<summary type="html">&lt;p&gt;Bo198214: added proposition A.1&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Shishikura writes&amp;lt;ref name=&amp;quot;Shishikura2000&amp;quot;&amp;gt;Shishikura, M. (2000). Bifurcation of parabolic fixed points. In Lei, Tan, The Mandelbrot set, theme and variations. Cambridge: Cambridge University Press. Lond. Math. Soc. Lect. Note Ser. 274, 325-363 (2000)&amp;lt;/ref&amp;gt; the following&lt;br /&gt;
&lt;br /&gt;
== $\mathcal{F}_0$ ==&lt;br /&gt;
&amp;amp;#91;p. 327&amp;amp;#93;&lt;br /&gt;
 &lt;br /&gt;
If $f_0&amp;#039;&amp;#039;(0)\neq 0$ by another coordinate change we may assume that $f_0&amp;#039;&amp;#039;(0)=1$, so define&lt;br /&gt;
$$ \mathcal{F}_0 = \{ f_0 \colon f_0 \quad\text{is defined and analytic in a neighborhood of 0}\quad f_0(0)=0, f_0&amp;#039;(0)=1, f_0&amp;#039;&amp;#039;(0)=1\}$$&lt;br /&gt;
&lt;br /&gt;
== Neighborhood of $f$ in the compact-open topology with domain of definition ==&lt;br /&gt;
&amp;amp;#91; p. 332 &amp;amp;#93;&lt;br /&gt;
&lt;br /&gt;
In what follows a map $f$ is always associated with its domain of definition $D(f)$. That is two maps are considered as distinct if they have distinct domains, even if the one is an extension of the other. A neighborhood of an analytic map $f\colon D(f)\to\overline{\C}$ is a set containing&lt;br /&gt;
$$\{ g \colon g \quad\text{is analytic},\quad D(g)\supset K, \sup_{z\in K} d(f(z)-g(z))&amp;lt;\eps \} $$&lt;br /&gt;
where $K$ is a compact set in $D(f)$, $\eps&amp;gt;0$ and $d(.,.)$ is the spherical metric.&lt;br /&gt;
A sequence $(f_n)$ converges to $f$ in this topology if and only if for any compact set $K\subset D(f)$ there exists $n_0$ such that $K\subset D(f_n)$ for all $n\ge n_0$ and $f_n|_K\to f|_K$ uniformly on $K$ as $n\to\infty$. The system of these neighborhoods define the &amp;quot;compact-open topology together with the domain of defintion&amp;quot;, which is unfortunately not Hausdorff, since an extension of $f$ is contained in any neighborhood of $f$.&lt;br /&gt;
&lt;br /&gt;
For $b_1,b_2\in\C$ with $\Re(b_1)&amp;lt;\Re(b_2)$ define &lt;br /&gt;
$$Q(b_1,b_2)=\{z\in\C\colon \Re(z-b_1)&amp;gt;-|\Im(z-b_1)|, \Re(z-b_2)&amp;gt;|\Im(z-b_2)|\}$$&lt;br /&gt;
If $b_1=-\infty$ (resp. $b_2=\infty$) then the corresponding condition should be removed.&lt;br /&gt;
&lt;br /&gt;
== Proposition 2.5.2 ==&lt;br /&gt;
&amp;amp;#91;p. 333&amp;amp;#93;&lt;br /&gt;
&lt;br /&gt;
Let $f$ be a holomorphic function defined on $Q=Q(b_1,b_2)$ with $\Re(b_2)&amp;gt;\Re(b_1)+2$ (here $b_1$ or $b_2$ may be $-\infty$ or $\infty$). Suppose &lt;br /&gt;
$$|F(z)-(z+1)|&amp;lt;\frac{1}{4},\quad |F&amp;#039;(z)-(z+1)|&amp;lt;\frac{1}{4}\quad \text{for all}\quad z\in Q.$$&lt;br /&gt;
&lt;br /&gt;
Then&lt;br /&gt;
# $F$ is univalent &amp;amp;#91;means injective&amp;amp;#93; on $Q$.&lt;br /&gt;
# Let $z_0\in Q$ be a point such that $\Re(b_1)&amp;lt;\Re(z_0)&amp;lt;\Re(b_2)-\frac{5}{4}$. Denote by $S$ the closed region (a strip) bounded by the two curves $\ell=\{z_0+i y\colon y\in\R\}$ and $F(\ell)$. Then for any $z\in Q$ there exist a unique $n\in \Z$ such that $F^n(z)$ is defined and belongs to $S-F(\ell)$.&lt;br /&gt;
# There exists an univalent function $\Phi\colon Q\to \C$ satisfying $$\Phi(F(z))=\Phi(z)+1$$ whenever both sides are defined. Moreover $\Phi$ is unique up to an addition of a constant.&lt;br /&gt;
# Fix a point $z_0\in Q$. If we normalize $\Phi$ by $\Phi(z_0)=0$ then the correspondence $F\mapsto \Phi$ is continuous with respect to the compact-open topology.&lt;br /&gt;
&lt;br /&gt;
== $\mathcal{F}$, $\mathcal{F}_1$ and $\alpha(f)$ ==&lt;br /&gt;
&amp;amp;#91;p. 339&amp;amp;#93;&lt;br /&gt;
&lt;br /&gt;
$$ \mathcal{F} = \{ f \colon f \quad\text{is defined and analytic in a neighborhood of 0}\quad f(0)=0, f_0&amp;#039;(0)\neq 0\}$$&lt;br /&gt;
For $f\in \mathcal{F}$ we express the derivative &lt;br /&gt;
$$f&amp;#039;(0)=\exp(2\pi i \alpha(f))$$&lt;br /&gt;
where $\alpha(f)\in\C$ and $-\frac{1}{2} &amp;lt; \Re(\alpha(f)) \le \frac{1}{2}$ our study is focussed on the maps in the following class&lt;br /&gt;
$$ \mathcal{F}_1 = \{ f\in \mathcal{F}\colon |\arg(\alpha(f))| &amp;lt; \frac{\pi}{4}\} $$&lt;br /&gt;
&lt;br /&gt;
=== Comments ===&lt;br /&gt;
&lt;br /&gt;
By the definition we have $$&lt;br /&gt;
\begin{align*}&lt;br /&gt;
\log(f&amp;#039;(0))&amp;amp;=2\pi i\alpha(f)=2\pi i re^{i\beta}=2\pi r e^{i(\beta+\frac{\pi}{2})}\\&lt;br /&gt;
\arg(\log(f&amp;#039;(0))&amp;amp;=\beta+\frac{\pi}{2}&lt;br /&gt;
\end{align*}$$&lt;br /&gt;
so the condition for $\mathcal{F}_1$ is&lt;br /&gt;
$|\arg(\log(f&amp;#039;(0)))-\frac{\pi}{2}|&amp;lt;\frac{\pi}{4}$ or&lt;br /&gt;
$$\frac{\pi}{4} &amp;lt; \arg(\log(f&amp;#039;(0)) &amp;lt; \frac{3\pi}{4}$$&lt;br /&gt;
&lt;br /&gt;
== $\sigma(f)$ ==&lt;br /&gt;
&amp;amp;#91;p. 340&amp;amp;#93;&lt;br /&gt;
&lt;br /&gt;
Let $\sigma(f)$ be the other fixpoint of $f$ (besides 0).&lt;br /&gt;
&lt;br /&gt;
...&lt;br /&gt;
&lt;br /&gt;
$$\sigma(f) = 2\pi i \alpha(f)(1+o(1)), \quad\text{as}\quad f\to f_0$$&lt;br /&gt;
&lt;br /&gt;
=== Comments ===&lt;br /&gt;
&lt;br /&gt;
By the comment before, we can say that $\sigma(f)$ lies roughly in the sector of angle $(\frac{\pi}{4},\frac{3\pi}{4})$ above the tip 0.&lt;br /&gt;
&lt;br /&gt;
== Proposition 3.2.2 ==&lt;br /&gt;
[p. 340]&lt;br /&gt;
&lt;br /&gt;
Let $f_0\in\mathcal{F}_0$. There exists a neighborhood $\mathcal{N}_0$ of $f_0$ (in the sense of the topology defined in 2.5.1) such that if $f\in\mathcal{N}_0\cap \mathcal{F}_1$, then there exist closed Jordan domains $S_{-,f}$, $S_{+,f}$ and analytic functions $\Phi_{-,f}$, $\Phi_{+,f}$ satisfying the following:&lt;br /&gt;
&lt;br /&gt;
(i) $S_{+,f}$ is bounded by an arc $\ell_{\pm}$ and its image $f(\ell_{\pm})$ such that $\ell_{\pm}$ joins two fixed points $\{0,\sigma(f)\}$, $\ell_{\pm}\cap f(\ell_{\pm}) = \{0,\sigma(f)\}$ and $S_{-,f}\cap S_{+,f} = \{0,\sigma(f)\}$; &lt;br /&gt;
&lt;br /&gt;
(ii) $\Phi_{\pm,f}$ is defined, analytic and injective in a neighborhood of $S&amp;#039;_{\pm,f} = S_{\pm,f}\setminus \{0,\sigma(f)\}$;&lt;br /&gt;
&lt;br /&gt;
(iii) if $z\in S&amp;#039;_{-,f}$ then there is an $n\ge 1$ such that $f^n(z)\in S&amp;#039;_{+,f}$ and for the smallest such $n$,&lt;br /&gt;
\[ \Phi_{+,f}(f^n(z)) = \Phi_{-,f}(z) - \frac{1}{\alpha(f)} + n \]&lt;br /&gt;
&lt;br /&gt;
(iv) when $f\in\mathcal{F}_1$ tends to $f_0$, $S_{\pm,f}\to S_{\pm,0}\cup \{0\}$ in the Hausdorff metric, and $\Phi_{\pm,f}\to \Phi_{\pm,0}$ in the topology defined in 2.5.1.&lt;br /&gt;
&lt;br /&gt;
== Proposition 4.4.1 ==&lt;br /&gt;
&amp;amp;#91;p. 356&amp;amp;#93;&lt;br /&gt;
&lt;br /&gt;
Let $f_0\in\mathcal{F}_0$, there exists a neighborhood $\mathcal{N}_0$ of $f_0$ (in the previously described &amp;quot;compact-open topology with domain of definition&amp;quot;), such that if $f\in \mathcal{N}_0 \cap \mathcal{F}_1$, then there exist large $\xi_0, \eta_0&amp;gt;0$, and analytic maps $\ph_f\colon D(\ph_f)\to\overline{\C}$ and $\tilde{\mathcal{R}}_f\colon D(\tilde{\mathcal{R}}_f)\to \C$ satisfying the following:&lt;br /&gt;
# $D(\ph_f)$ contains the set $$ \mathcal{Q}_f = \{ w\in\C\colon |\arg(-w-\xi_0)| &amp;lt; \frac{2\pi}{3}, |\arg(w+\frac{1}{\alpha(f)}-\xi_0)|&amp;lt;\frac{2\pi}{3} \} $$ and $\ph_f(D(\ph_f)) \subseteq D(f)$; If $w, w+1\in D(\ph_f)$ then $$ \ph_f(w+1)=f(\ph_f(w)) $$ $\ph_f(w)\to 0$ when $w\in \mathcal{Q}_f$ and $\Im(w)\to\infty$; $\ph_f(w)\to\sigma(f)$ when $w\in\mathcal{Q}_f$ and $\Im(w)\to -\infty$.&lt;br /&gt;
# $D(\tilde{\mathcal{R}}_f)$ contains $\{ w\in\C\colon |\Im(w)| &amp;gt; \eta_0\}$ and is invariant under $T(w)=w+1$; if $w\in D(\tilde{\mathcal{R}}_f)$ then $$\tilde{\mathcal{R}}_f(w+1)=\tilde{\mathcal{R}}(w)+1;$$ $\tilde{\mathcal{R}}_f(w)-w$ tends to $-\frac{1}{\alpha(f)}$ when $\Im(w)\to\infty$; to a constant when $\Im(w)\to -\infty$.&lt;br /&gt;
# If $w\in D(\tilde{\mathcal{R}}_f)\cap D(\ph_f)$ and $w&amp;#039;=\tilde{\mathcal{R}}_f(w)+n\in D(\ph_f)$ for some $n\in\Z$ then $$f^n(\ph_f(w))=\ph_f(w&amp;#039;)\quad \text{for}\quad n\ge 0, \quad f^{-n}(\ph_f(w&amp;#039;))=\ph_f(w)\quad \text{for}\quad n&amp;lt;0$$ Moreover if $|\arg(w&amp;#039;+\frac{1}{2\alpha(f)}-\xi_0)|&amp;lt;\frac{2\pi}{3}$ then $n&amp;gt;0$.&lt;br /&gt;
# When $f\in\mathcal{F_1}$ and $f\to f_0$ $$\ph_f\to\ph_0\quad\text{and}\quad \tilde{\mathcal{R}}_f + \frac{1}{\alpha(f)} \to \tilde{\mathcal{E}}_{f_0}$$&lt;br /&gt;
&lt;br /&gt;
== Proposition A.1 ==&lt;br /&gt;
&lt;br /&gt;
&amp;lt;references/&amp;gt;&lt;/div&gt;</summary>
		<author><name>Bo198214</name></author>
	</entry>
	<entry>
		<id>https://tetrationforum.org/hyperops_wiki/index.php?title=Shishikura_perturbed_Fatou_coordinates&amp;diff=150</id>
		<title>Shishikura perturbed Fatou coordinates</title>
		<link rel="alternate" type="text/html" href="https://tetrationforum.org/hyperops_wiki/index.php?title=Shishikura_perturbed_Fatou_coordinates&amp;diff=150"/>
		<updated>2013-02-19T21:39:06Z</updated>

		<summary type="html">&lt;p&gt;Bo198214: /* Proposition 3.2.2 */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Shishikura writes&amp;lt;ref name=&amp;quot;Shishikura2000&amp;quot;&amp;gt;Shishikura, M. (2000). Bifurcation of parabolic fixed points. In Lei, Tan, The Mandelbrot set, theme and variations. Cambridge: Cambridge University Press. Lond. Math. Soc. Lect. Note Ser. 274, 325-363 (2000)&amp;lt;/ref&amp;gt; the following&lt;br /&gt;
&lt;br /&gt;
== $\mathcal{F}_0$ ==&lt;br /&gt;
&amp;amp;#91;p. 327&amp;amp;#93;&lt;br /&gt;
 &lt;br /&gt;
If $f_0&amp;#039;&amp;#039;(0)\neq 0$ by another coordinate change we may assume that $f_0&amp;#039;&amp;#039;(0)=1$, so define&lt;br /&gt;
$$ \mathcal{F}_0 = \{ f_0 \colon f_0 \quad\text{is defined and analytic in a neighborhood of 0}\quad f_0(0)=0, f_0&amp;#039;(0)=1, f_0&amp;#039;&amp;#039;(0)=1\}$$&lt;br /&gt;
&lt;br /&gt;
== Neighborhood of $f$ in the compact-open topology with domain of definition ==&lt;br /&gt;
&amp;amp;#91; p. 332 &amp;amp;#93;&lt;br /&gt;
&lt;br /&gt;
In what follows a map $f$ is always associated with its domain of definition $D(f)$. That is two maps are considered as distinct if they have distinct domains, even if the one is an extension of the other. A neighborhood of an analytic map $f\colon D(f)\to\overline{\C}$ is a set containing&lt;br /&gt;
$$\{ g \colon g \quad\text{is analytic},\quad D(g)\supset K, \sup_{z\in K} d(f(z)-g(z))&amp;lt;\eps \} $$&lt;br /&gt;
where $K$ is a compact set in $D(f)$, $\eps&amp;gt;0$ and $d(.,.)$ is the spherical metric.&lt;br /&gt;
A sequence $(f_n)$ converges to $f$ in this topology if and only if for any compact set $K\subset D(f)$ there exists $n_0$ such that $K\subset D(f_n)$ for all $n\ge n_0$ and $f_n|_K\to f|_K$ uniformly on $K$ as $n\to\infty$. The system of these neighborhoods define the &amp;quot;compact-open topology together with the domain of defintion&amp;quot;, which is unfortunately not Hausdorff, since an extension of $f$ is contained in any neighborhood of $f$.&lt;br /&gt;
&lt;br /&gt;
For $b_1,b_2\in\C$ with $\Re(b_1)&amp;lt;\Re(b_2)$ define &lt;br /&gt;
$$Q(b_1,b_2)=\{z\in\C\colon \Re(z-b_1)&amp;gt;-|\Im(z-b_1)|, \Re(z-b_2)&amp;gt;|\Im(z-b_2)|\}$$&lt;br /&gt;
If $b_1=-\infty$ (resp. $b_2=\infty$) then the corresponding condition should be removed.&lt;br /&gt;
&lt;br /&gt;
== Proposition 2.5.2 ==&lt;br /&gt;
&amp;amp;#91;p. 333&amp;amp;#93;&lt;br /&gt;
&lt;br /&gt;
Let $f$ be a holomorphic function defined on $Q=Q(b_1,b_2)$ with $\Re(b_2)&amp;gt;\Re(b_1)+2$ (here $b_1$ or $b_2$ may be $-\infty$ or $\infty$). Suppose &lt;br /&gt;
$$|F(z)-(z+1)|&amp;lt;\frac{1}{4},\quad |F&amp;#039;(z)-(z+1)|&amp;lt;\frac{1}{4}\quad \text{for all}\quad z\in Q.$$&lt;br /&gt;
&lt;br /&gt;
Then&lt;br /&gt;
# $F$ is univalent &amp;amp;#91;means injective&amp;amp;#93; on $Q$.&lt;br /&gt;
# Let $z_0\in Q$ be a point such that $\Re(b_1)&amp;lt;\Re(z_0)&amp;lt;\Re(b_2)-\frac{5}{4}$. Denote by $S$ the closed region (a strip) bounded by the two curves $\ell=\{z_0+i y\colon y\in\R\}$ and $F(\ell)$. Then for any $z\in Q$ there exist a unique $n\in \Z$ such that $F^n(z)$ is defined and belongs to $S-F(\ell)$.&lt;br /&gt;
# There exists an univalent function $\Phi\colon Q\to \C$ satisfying $$\Phi(F(z))=\Phi(z)+1$$ whenever both sides are defined. Moreover $\Phi$ is unique up to an addition of a constant.&lt;br /&gt;
# Fix a point $z_0\in Q$. If we normalize $\Phi$ by $\Phi(z_0)=0$ then the correspondence $F\mapsto \Phi$ is continuous with respect to the compact-open topology.&lt;br /&gt;
&lt;br /&gt;
== $\mathcal{F}$, $\mathcal{F}_1$ and $\alpha(f)$ ==&lt;br /&gt;
&amp;amp;#91;p. 339&amp;amp;#93;&lt;br /&gt;
&lt;br /&gt;
$$ \mathcal{F} = \{ f \colon f \quad\text{is defined and analytic in a neighborhood of 0}\quad f(0)=0, f_0&amp;#039;(0)\neq 0\}$$&lt;br /&gt;
For $f\in \mathcal{F}$ we express the derivative &lt;br /&gt;
$$f&amp;#039;(0)=\exp(2\pi i \alpha(f))$$&lt;br /&gt;
where $\alpha(f)\in\C$ and $-\frac{1}{2} &amp;lt; \Re(\alpha(f)) \le \frac{1}{2}$ our study is focussed on the maps in the following class&lt;br /&gt;
$$ \mathcal{F}_1 = \{ f\in \mathcal{F}\colon |\arg(\alpha(f))| &amp;lt; \frac{\pi}{4}\} $$&lt;br /&gt;
&lt;br /&gt;
=== Comments ===&lt;br /&gt;
&lt;br /&gt;
By the definition we have $$&lt;br /&gt;
\begin{align*}&lt;br /&gt;
\log(f&amp;#039;(0))&amp;amp;=2\pi i\alpha(f)=2\pi i re^{i\beta}=2\pi r e^{i(\beta+\frac{\pi}{2})}\\&lt;br /&gt;
\arg(\log(f&amp;#039;(0))&amp;amp;=\beta+\frac{\pi}{2}&lt;br /&gt;
\end{align*}$$&lt;br /&gt;
so the condition for $\mathcal{F}_1$ is&lt;br /&gt;
$|\arg(\log(f&amp;#039;(0)))-\frac{\pi}{2}|&amp;lt;\frac{\pi}{4}$ or&lt;br /&gt;
$$\frac{\pi}{4} &amp;lt; \arg(\log(f&amp;#039;(0)) &amp;lt; \frac{3\pi}{4}$$&lt;br /&gt;
&lt;br /&gt;
== $\sigma(f)$ ==&lt;br /&gt;
&amp;amp;#91;p. 340&amp;amp;#93;&lt;br /&gt;
&lt;br /&gt;
Let $\sigma(f)$ be the other fixpoint of $f$ (besides 0).&lt;br /&gt;
&lt;br /&gt;
...&lt;br /&gt;
&lt;br /&gt;
$$\sigma(f) = 2\pi i \alpha(f)(1+o(1)), \quad\text{as}\quad f\to f_0$$&lt;br /&gt;
&lt;br /&gt;
=== Comments ===&lt;br /&gt;
&lt;br /&gt;
By the comment before, we can say that $\sigma(f)$ lies roughly in the sector of angle $(\frac{\pi}{4},\frac{3\pi}{4})$ above the tip 0.&lt;br /&gt;
&lt;br /&gt;
== Proposition 3.2.2 ==&lt;br /&gt;
[p. 340]&lt;br /&gt;
&lt;br /&gt;
Let $f_0\in\mathcal{F}_0$. There exists a neighborhood $\mathcal{N}_0$ of $f_0$ (in the sense of the topology defined in 2.5.1) such that if $f\in\mathcal{N}_0\cap \mathcal{F}_1$, then there exist closed Jordan domains $S_{-,f}$, $S_{+,f}$ and analytic functions $\Phi_{-,f}$, $\Phi_{+,f}$ satisfying the following:&lt;br /&gt;
&lt;br /&gt;
(i) $S_{+,f}$ is bounded by an arc $\ell_{\pm}$ and its image $f(\ell_{\pm})$ such that $\ell_{\pm}$ joins two fixed points $\{0,\sigma(f)\}$, $\ell_{\pm}\cap f(\ell_{\pm}) = \{0,\sigma(f)\}$ and $S_{-,f}\cap S_{+,f} = \{0,\sigma(f)\}$; &lt;br /&gt;
&lt;br /&gt;
(ii) $\Phi_{\pm,f}$ is defined, analytic and injective in a neighborhood of $S&amp;#039;_{\pm,f} = S_{\pm,f}\setminus \{0,\sigma(f)\}$;&lt;br /&gt;
&lt;br /&gt;
(iii) if $z\in S&amp;#039;_{-,f}$ then there is an $n\ge 1$ such that $f^n(z)\in S&amp;#039;_{+,f}$ and for the smallest such $n$,&lt;br /&gt;
\[ \Phi_{+,f}(f^n(z)) = \Phi_{-,f}(z) - \frac{1}{\alpha(f)} + n \]&lt;br /&gt;
&lt;br /&gt;
(iv) when $f\in\mathcal{F}_1$ tends to $f_0$, $S_{\pm,f}\to S_{\pm,0}\cup \{0\}$ in the Hausdorff metric, and $\Phi_{\pm,f}\to \Phi_{\pm,0}$ in the topology defined in 2.5.1.&lt;br /&gt;
&lt;br /&gt;
== Proposition 4.4.1 ==&lt;br /&gt;
&amp;amp;#91;p. 356&amp;amp;#93;&lt;br /&gt;
&lt;br /&gt;
Let $f_0\in\mathcal{F}_0$, there exists a neighborhood $\mathcal{N}_0$ of $f_0$ (in the previously described &amp;quot;compact-open topology with domain of definition&amp;quot;), such that if $f\in \mathcal{N}_0 \cap \mathcal{F}_1$, then there exist large $\xi_0, \eta_0&amp;gt;0$, and analytic maps $\ph_f\colon D(\ph_f)\to\overline{\C}$ and $\tilde{\mathcal{R}}_f\colon D(\tilde{\mathcal{R}}_f)\to \C$ satisfying the following:&lt;br /&gt;
# $D(\ph_f)$ contains the set $$ \mathcal{Q}_f = \{ w\in\C\colon |\arg(-w-\xi_0)| &amp;lt; \frac{2\pi}{3}, |\arg(w+\frac{1}{\alpha(f)}-\xi_0)|&amp;lt;\frac{2\pi}{3} \} $$ and $\ph_f(D(\ph_f)) \subseteq D(f)$; If $w, w+1\in D(\ph_f)$ then $$ \ph_f(w+1)=f(\ph_f(w)) $$ $\ph_f(w)\to 0$ when $w\in \mathcal{Q}_f$ and $\Im(w)\to\infty$; $\ph_f(w)\to\sigma(f)$ when $w\in\mathcal{Q}_f$ and $\Im(w)\to -\infty$.&lt;br /&gt;
# $D(\tilde{\mathcal{R}}_f)$ contains $\{ w\in\C\colon |\Im(w)| &amp;gt; \eta_0\}$ and is invariant under $T(w)=w+1$; if $w\in D(\tilde{\mathcal{R}}_f)$ then $$\tilde{\mathcal{R}}_f(w+1)=\tilde{\mathcal{R}}(w)+1;$$ $\tilde{\mathcal{R}}_f(w)-w$ tends to $-\frac{1}{\alpha(f)}$ when $\Im(w)\to\infty$; to a constant when $\Im(w)\to -\infty$.&lt;br /&gt;
# If $w\in D(\tilde{\mathcal{R}}_f)\cap D(\ph_f)$ and $w&amp;#039;=\tilde{\mathcal{R}}_f(w)+n\in D(\ph_f)$ for some $n\in\Z$ then $$f^n(\ph_f(w))=\ph_f(w&amp;#039;)\quad \text{for}\quad n\ge 0, \quad f^{-n}(\ph_f(w&amp;#039;))=\ph_f(w)\quad \text{for}\quad n&amp;lt;0$$ Moreover if $|\arg(w&amp;#039;+\frac{1}{2\alpha(f)}-\xi_0)|&amp;lt;\frac{2\pi}{3}$ then $n&amp;gt;0$.&lt;br /&gt;
# When $f\in\mathcal{F_1}$ and $f\to f_0$ $$\ph_f\to\ph_0\quad\text{and}\quad \tilde{\mathcal{R}}_f + \frac{1}{\alpha(f)} \to \tilde{\mathcal{E}}_{f_0}$$&lt;br /&gt;
&lt;br /&gt;
&amp;lt;references/&amp;gt;&lt;/div&gt;</summary>
		<author><name>Bo198214</name></author>
	</entry>
	<entry>
		<id>https://tetrationforum.org/hyperops_wiki/index.php?title=Shishikura_perturbed_Fatou_coordinates&amp;diff=149</id>
		<title>Shishikura perturbed Fatou coordinates</title>
		<link rel="alternate" type="text/html" href="https://tetrationforum.org/hyperops_wiki/index.php?title=Shishikura_perturbed_Fatou_coordinates&amp;diff=149"/>
		<updated>2013-02-19T21:38:40Z</updated>

		<summary type="html">&lt;p&gt;Bo198214: /* Proposition 3.2.2 */ added page number&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Shishikura writes&amp;lt;ref name=&amp;quot;Shishikura2000&amp;quot;&amp;gt;Shishikura, M. (2000). Bifurcation of parabolic fixed points. In Lei, Tan, The Mandelbrot set, theme and variations. Cambridge: Cambridge University Press. Lond. Math. Soc. Lect. Note Ser. 274, 325-363 (2000)&amp;lt;/ref&amp;gt; the following&lt;br /&gt;
&lt;br /&gt;
== $\mathcal{F}_0$ ==&lt;br /&gt;
&amp;amp;#91;p. 327&amp;amp;#93;&lt;br /&gt;
 &lt;br /&gt;
If $f_0&amp;#039;&amp;#039;(0)\neq 0$ by another coordinate change we may assume that $f_0&amp;#039;&amp;#039;(0)=1$, so define&lt;br /&gt;
$$ \mathcal{F}_0 = \{ f_0 \colon f_0 \quad\text{is defined and analytic in a neighborhood of 0}\quad f_0(0)=0, f_0&amp;#039;(0)=1, f_0&amp;#039;&amp;#039;(0)=1\}$$&lt;br /&gt;
&lt;br /&gt;
== Neighborhood of $f$ in the compact-open topology with domain of definition ==&lt;br /&gt;
&amp;amp;#91; p. 332 &amp;amp;#93;&lt;br /&gt;
&lt;br /&gt;
In what follows a map $f$ is always associated with its domain of definition $D(f)$. That is two maps are considered as distinct if they have distinct domains, even if the one is an extension of the other. A neighborhood of an analytic map $f\colon D(f)\to\overline{\C}$ is a set containing&lt;br /&gt;
$$\{ g \colon g \quad\text{is analytic},\quad D(g)\supset K, \sup_{z\in K} d(f(z)-g(z))&amp;lt;\eps \} $$&lt;br /&gt;
where $K$ is a compact set in $D(f)$, $\eps&amp;gt;0$ and $d(.,.)$ is the spherical metric.&lt;br /&gt;
A sequence $(f_n)$ converges to $f$ in this topology if and only if for any compact set $K\subset D(f)$ there exists $n_0$ such that $K\subset D(f_n)$ for all $n\ge n_0$ and $f_n|_K\to f|_K$ uniformly on $K$ as $n\to\infty$. The system of these neighborhoods define the &amp;quot;compact-open topology together with the domain of defintion&amp;quot;, which is unfortunately not Hausdorff, since an extension of $f$ is contained in any neighborhood of $f$.&lt;br /&gt;
&lt;br /&gt;
For $b_1,b_2\in\C$ with $\Re(b_1)&amp;lt;\Re(b_2)$ define &lt;br /&gt;
$$Q(b_1,b_2)=\{z\in\C\colon \Re(z-b_1)&amp;gt;-|\Im(z-b_1)|, \Re(z-b_2)&amp;gt;|\Im(z-b_2)|\}$$&lt;br /&gt;
If $b_1=-\infty$ (resp. $b_2=\infty$) then the corresponding condition should be removed.&lt;br /&gt;
&lt;br /&gt;
== Proposition 2.5.2 ==&lt;br /&gt;
&amp;amp;#91;p. 333&amp;amp;#93;&lt;br /&gt;
&lt;br /&gt;
Let $f$ be a holomorphic function defined on $Q=Q(b_1,b_2)$ with $\Re(b_2)&amp;gt;\Re(b_1)+2$ (here $b_1$ or $b_2$ may be $-\infty$ or $\infty$). Suppose &lt;br /&gt;
$$|F(z)-(z+1)|&amp;lt;\frac{1}{4},\quad |F&amp;#039;(z)-(z+1)|&amp;lt;\frac{1}{4}\quad \text{for all}\quad z\in Q.$$&lt;br /&gt;
&lt;br /&gt;
Then&lt;br /&gt;
# $F$ is univalent &amp;amp;#91;means injective&amp;amp;#93; on $Q$.&lt;br /&gt;
# Let $z_0\in Q$ be a point such that $\Re(b_1)&amp;lt;\Re(z_0)&amp;lt;\Re(b_2)-\frac{5}{4}$. Denote by $S$ the closed region (a strip) bounded by the two curves $\ell=\{z_0+i y\colon y\in\R\}$ and $F(\ell)$. Then for any $z\in Q$ there exist a unique $n\in \Z$ such that $F^n(z)$ is defined and belongs to $S-F(\ell)$.&lt;br /&gt;
# There exists an univalent function $\Phi\colon Q\to \C$ satisfying $$\Phi(F(z))=\Phi(z)+1$$ whenever both sides are defined. Moreover $\Phi$ is unique up to an addition of a constant.&lt;br /&gt;
# Fix a point $z_0\in Q$. If we normalize $\Phi$ by $\Phi(z_0)=0$ then the correspondence $F\mapsto \Phi$ is continuous with respect to the compact-open topology.&lt;br /&gt;
&lt;br /&gt;
== $\mathcal{F}$, $\mathcal{F}_1$ and $\alpha(f)$ ==&lt;br /&gt;
&amp;amp;#91;p. 339&amp;amp;#93;&lt;br /&gt;
&lt;br /&gt;
$$ \mathcal{F} = \{ f \colon f \quad\text{is defined and analytic in a neighborhood of 0}\quad f(0)=0, f_0&amp;#039;(0)\neq 0\}$$&lt;br /&gt;
For $f\in \mathcal{F}$ we express the derivative &lt;br /&gt;
$$f&amp;#039;(0)=\exp(2\pi i \alpha(f))$$&lt;br /&gt;
where $\alpha(f)\in\C$ and $-\frac{1}{2} &amp;lt; \Re(\alpha(f)) \le \frac{1}{2}$ our study is focussed on the maps in the following class&lt;br /&gt;
$$ \mathcal{F}_1 = \{ f\in \mathcal{F}\colon |\arg(\alpha(f))| &amp;lt; \frac{\pi}{4}\} $$&lt;br /&gt;
&lt;br /&gt;
=== Comments ===&lt;br /&gt;
&lt;br /&gt;
By the definition we have $$&lt;br /&gt;
\begin{align*}&lt;br /&gt;
\log(f&amp;#039;(0))&amp;amp;=2\pi i\alpha(f)=2\pi i re^{i\beta}=2\pi r e^{i(\beta+\frac{\pi}{2})}\\&lt;br /&gt;
\arg(\log(f&amp;#039;(0))&amp;amp;=\beta+\frac{\pi}{2}&lt;br /&gt;
\end{align*}$$&lt;br /&gt;
so the condition for $\mathcal{F}_1$ is&lt;br /&gt;
$|\arg(\log(f&amp;#039;(0)))-\frac{\pi}{2}|&amp;lt;\frac{\pi}{4}$ or&lt;br /&gt;
$$\frac{\pi}{4} &amp;lt; \arg(\log(f&amp;#039;(0)) &amp;lt; \frac{3\pi}{4}$$&lt;br /&gt;
&lt;br /&gt;
== $\sigma(f)$ ==&lt;br /&gt;
&amp;amp;#91;p. 340&amp;amp;#93;&lt;br /&gt;
&lt;br /&gt;
Let $\sigma(f)$ be the other fixpoint of $f$ (besides 0).&lt;br /&gt;
&lt;br /&gt;
...&lt;br /&gt;
&lt;br /&gt;
$$\sigma(f) = 2\pi i \alpha(f)(1+o(1)), \quad\text{as}\quad f\to f_0$$&lt;br /&gt;
&lt;br /&gt;
=== Comments ===&lt;br /&gt;
&lt;br /&gt;
By the comment before, we can say that $\sigma(f)$ lies roughly in the sector of angle $(\frac{\pi}{4},\frac{3\pi}{4})$ above the tip 0.&lt;br /&gt;
&lt;br /&gt;
== Proposition 3.2.2 ==&lt;br /&gt;
[p. 340]&lt;br /&gt;
Let $f_0\in\mathcal{F}_0$. There exists a neighborhood $\mathcal{N}_0$ of $f_0$ (in the sense of the topology defined in 2.5.1) such that if $f\in\mathcal{N}_0\cap \mathcal{F}_1$, then there exist closed Jordan domains $S_{-,f}$, $S_{+,f}$ and analytic functions $\Phi_{-,f}$, $\Phi_{+,f}$ satisfying the following:&lt;br /&gt;
&lt;br /&gt;
(i) $S_{+,f}$ is bounded by an arc $\ell_{\pm}$ and its image $f(\ell_{\pm})$ such that $\ell_{\pm}$ joins two fixed points $\{0,\sigma(f)\}$, $\ell_{\pm}\cap f(\ell_{\pm}) = \{0,\sigma(f)\}$ and $S_{-,f}\cap S_{+,f} = \{0,\sigma(f)\}$; &lt;br /&gt;
&lt;br /&gt;
(ii) $\Phi_{\pm,f}$ is defined, analytic and injective in a neighborhood of $S&amp;#039;_{\pm,f} = S_{\pm,f}\setminus \{0,\sigma(f)\}$;&lt;br /&gt;
&lt;br /&gt;
(iii) if $z\in S&amp;#039;_{-,f}$ then there is an $n\ge 1$ such that $f^n(z)\in S&amp;#039;_{+,f}$ and for the smallest such $n$,&lt;br /&gt;
\[ \Phi_{+,f}(f^n(z)) = \Phi_{-,f}(z) - \frac{1}{\alpha(f)} + n \]&lt;br /&gt;
&lt;br /&gt;
(iv) when $f\in\mathcal{F}_1$ tends to $f_0$, $S_{\pm,f}\to S_{\pm,0}\cup \{0\}$ in the Hausdorff metric, and $\Phi_{\pm,f}\to \Phi_{\pm,0}$ in the topology defined in 2.5.1.&lt;br /&gt;
&lt;br /&gt;
== Proposition 4.4.1 ==&lt;br /&gt;
&amp;amp;#91;p. 356&amp;amp;#93;&lt;br /&gt;
&lt;br /&gt;
Let $f_0\in\mathcal{F}_0$, there exists a neighborhood $\mathcal{N}_0$ of $f_0$ (in the previously described &amp;quot;compact-open topology with domain of definition&amp;quot;), such that if $f\in \mathcal{N}_0 \cap \mathcal{F}_1$, then there exist large $\xi_0, \eta_0&amp;gt;0$, and analytic maps $\ph_f\colon D(\ph_f)\to\overline{\C}$ and $\tilde{\mathcal{R}}_f\colon D(\tilde{\mathcal{R}}_f)\to \C$ satisfying the following:&lt;br /&gt;
# $D(\ph_f)$ contains the set $$ \mathcal{Q}_f = \{ w\in\C\colon |\arg(-w-\xi_0)| &amp;lt; \frac{2\pi}{3}, |\arg(w+\frac{1}{\alpha(f)}-\xi_0)|&amp;lt;\frac{2\pi}{3} \} $$ and $\ph_f(D(\ph_f)) \subseteq D(f)$; If $w, w+1\in D(\ph_f)$ then $$ \ph_f(w+1)=f(\ph_f(w)) $$ $\ph_f(w)\to 0$ when $w\in \mathcal{Q}_f$ and $\Im(w)\to\infty$; $\ph_f(w)\to\sigma(f)$ when $w\in\mathcal{Q}_f$ and $\Im(w)\to -\infty$.&lt;br /&gt;
# $D(\tilde{\mathcal{R}}_f)$ contains $\{ w\in\C\colon |\Im(w)| &amp;gt; \eta_0\}$ and is invariant under $T(w)=w+1$; if $w\in D(\tilde{\mathcal{R}}_f)$ then $$\tilde{\mathcal{R}}_f(w+1)=\tilde{\mathcal{R}}(w)+1;$$ $\tilde{\mathcal{R}}_f(w)-w$ tends to $-\frac{1}{\alpha(f)}$ when $\Im(w)\to\infty$; to a constant when $\Im(w)\to -\infty$.&lt;br /&gt;
# If $w\in D(\tilde{\mathcal{R}}_f)\cap D(\ph_f)$ and $w&amp;#039;=\tilde{\mathcal{R}}_f(w)+n\in D(\ph_f)$ for some $n\in\Z$ then $$f^n(\ph_f(w))=\ph_f(w&amp;#039;)\quad \text{for}\quad n\ge 0, \quad f^{-n}(\ph_f(w&amp;#039;))=\ph_f(w)\quad \text{for}\quad n&amp;lt;0$$ Moreover if $|\arg(w&amp;#039;+\frac{1}{2\alpha(f)}-\xi_0)|&amp;lt;\frac{2\pi}{3}$ then $n&amp;gt;0$.&lt;br /&gt;
# When $f\in\mathcal{F_1}$ and $f\to f_0$ $$\ph_f\to\ph_0\quad\text{and}\quad \tilde{\mathcal{R}}_f + \frac{1}{\alpha(f)} \to \tilde{\mathcal{E}}_{f_0}$$&lt;br /&gt;
&lt;br /&gt;
&amp;lt;references/&amp;gt;&lt;/div&gt;</summary>
		<author><name>Bo198214</name></author>
	</entry>
	<entry>
		<id>https://tetrationforum.org/hyperops_wiki/index.php?title=Shishikura_perturbed_Fatou_coordinates&amp;diff=148</id>
		<title>Shishikura perturbed Fatou coordinates</title>
		<link rel="alternate" type="text/html" href="https://tetrationforum.org/hyperops_wiki/index.php?title=Shishikura_perturbed_Fatou_coordinates&amp;diff=148"/>
		<updated>2013-02-19T21:35:34Z</updated>

		<summary type="html">&lt;p&gt;Bo198214: /* Proposition 3.2.2 */ fixed some TeX&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Shishikura writes&amp;lt;ref name=&amp;quot;Shishikura2000&amp;quot;&amp;gt;Shishikura, M. (2000). Bifurcation of parabolic fixed points. In Lei, Tan, The Mandelbrot set, theme and variations. Cambridge: Cambridge University Press. Lond. Math. Soc. Lect. Note Ser. 274, 325-363 (2000)&amp;lt;/ref&amp;gt; the following&lt;br /&gt;
&lt;br /&gt;
== $\mathcal{F}_0$ ==&lt;br /&gt;
&amp;amp;#91;p. 327&amp;amp;#93;&lt;br /&gt;
 &lt;br /&gt;
If $f_0&amp;#039;&amp;#039;(0)\neq 0$ by another coordinate change we may assume that $f_0&amp;#039;&amp;#039;(0)=1$, so define&lt;br /&gt;
$$ \mathcal{F}_0 = \{ f_0 \colon f_0 \quad\text{is defined and analytic in a neighborhood of 0}\quad f_0(0)=0, f_0&amp;#039;(0)=1, f_0&amp;#039;&amp;#039;(0)=1\}$$&lt;br /&gt;
&lt;br /&gt;
== Neighborhood of $f$ in the compact-open topology with domain of definition ==&lt;br /&gt;
&amp;amp;#91; p. 332 &amp;amp;#93;&lt;br /&gt;
&lt;br /&gt;
In what follows a map $f$ is always associated with its domain of definition $D(f)$. That is two maps are considered as distinct if they have distinct domains, even if the one is an extension of the other. A neighborhood of an analytic map $f\colon D(f)\to\overline{\C}$ is a set containing&lt;br /&gt;
$$\{ g \colon g \quad\text{is analytic},\quad D(g)\supset K, \sup_{z\in K} d(f(z)-g(z))&amp;lt;\eps \} $$&lt;br /&gt;
where $K$ is a compact set in $D(f)$, $\eps&amp;gt;0$ and $d(.,.)$ is the spherical metric.&lt;br /&gt;
A sequence $(f_n)$ converges to $f$ in this topology if and only if for any compact set $K\subset D(f)$ there exists $n_0$ such that $K\subset D(f_n)$ for all $n\ge n_0$ and $f_n|_K\to f|_K$ uniformly on $K$ as $n\to\infty$. The system of these neighborhoods define the &amp;quot;compact-open topology together with the domain of defintion&amp;quot;, which is unfortunately not Hausdorff, since an extension of $f$ is contained in any neighborhood of $f$.&lt;br /&gt;
&lt;br /&gt;
For $b_1,b_2\in\C$ with $\Re(b_1)&amp;lt;\Re(b_2)$ define &lt;br /&gt;
$$Q(b_1,b_2)=\{z\in\C\colon \Re(z-b_1)&amp;gt;-|\Im(z-b_1)|, \Re(z-b_2)&amp;gt;|\Im(z-b_2)|\}$$&lt;br /&gt;
If $b_1=-\infty$ (resp. $b_2=\infty$) then the corresponding condition should be removed.&lt;br /&gt;
&lt;br /&gt;
== Proposition 2.5.2 ==&lt;br /&gt;
&amp;amp;#91;p. 333&amp;amp;#93;&lt;br /&gt;
&lt;br /&gt;
Let $f$ be a holomorphic function defined on $Q=Q(b_1,b_2)$ with $\Re(b_2)&amp;gt;\Re(b_1)+2$ (here $b_1$ or $b_2$ may be $-\infty$ or $\infty$). Suppose &lt;br /&gt;
$$|F(z)-(z+1)|&amp;lt;\frac{1}{4},\quad |F&amp;#039;(z)-(z+1)|&amp;lt;\frac{1}{4}\quad \text{for all}\quad z\in Q.$$&lt;br /&gt;
&lt;br /&gt;
Then&lt;br /&gt;
# $F$ is univalent &amp;amp;#91;means injective&amp;amp;#93; on $Q$.&lt;br /&gt;
# Let $z_0\in Q$ be a point such that $\Re(b_1)&amp;lt;\Re(z_0)&amp;lt;\Re(b_2)-\frac{5}{4}$. Denote by $S$ the closed region (a strip) bounded by the two curves $\ell=\{z_0+i y\colon y\in\R\}$ and $F(\ell)$. Then for any $z\in Q$ there exist a unique $n\in \Z$ such that $F^n(z)$ is defined and belongs to $S-F(\ell)$.&lt;br /&gt;
# There exists an univalent function $\Phi\colon Q\to \C$ satisfying $$\Phi(F(z))=\Phi(z)+1$$ whenever both sides are defined. Moreover $\Phi$ is unique up to an addition of a constant.&lt;br /&gt;
# Fix a point $z_0\in Q$. If we normalize $\Phi$ by $\Phi(z_0)=0$ then the correspondence $F\mapsto \Phi$ is continuous with respect to the compact-open topology.&lt;br /&gt;
&lt;br /&gt;
== $\mathcal{F}$, $\mathcal{F}_1$ and $\alpha(f)$ ==&lt;br /&gt;
&amp;amp;#91;p. 339&amp;amp;#93;&lt;br /&gt;
&lt;br /&gt;
$$ \mathcal{F} = \{ f \colon f \quad\text{is defined and analytic in a neighborhood of 0}\quad f(0)=0, f_0&amp;#039;(0)\neq 0\}$$&lt;br /&gt;
For $f\in \mathcal{F}$ we express the derivative &lt;br /&gt;
$$f&amp;#039;(0)=\exp(2\pi i \alpha(f))$$&lt;br /&gt;
where $\alpha(f)\in\C$ and $-\frac{1}{2} &amp;lt; \Re(\alpha(f)) \le \frac{1}{2}$ our study is focussed on the maps in the following class&lt;br /&gt;
$$ \mathcal{F}_1 = \{ f\in \mathcal{F}\colon |\arg(\alpha(f))| &amp;lt; \frac{\pi}{4}\} $$&lt;br /&gt;
&lt;br /&gt;
=== Comments ===&lt;br /&gt;
&lt;br /&gt;
By the definition we have $$&lt;br /&gt;
\begin{align*}&lt;br /&gt;
\log(f&amp;#039;(0))&amp;amp;=2\pi i\alpha(f)=2\pi i re^{i\beta}=2\pi r e^{i(\beta+\frac{\pi}{2})}\\&lt;br /&gt;
\arg(\log(f&amp;#039;(0))&amp;amp;=\beta+\frac{\pi}{2}&lt;br /&gt;
\end{align*}$$&lt;br /&gt;
so the condition for $\mathcal{F}_1$ is&lt;br /&gt;
$|\arg(\log(f&amp;#039;(0)))-\frac{\pi}{2}|&amp;lt;\frac{\pi}{4}$ or&lt;br /&gt;
$$\frac{\pi}{4} &amp;lt; \arg(\log(f&amp;#039;(0)) &amp;lt; \frac{3\pi}{4}$$&lt;br /&gt;
&lt;br /&gt;
== $\sigma(f)$ ==&lt;br /&gt;
&amp;amp;#91;p. 340&amp;amp;#93;&lt;br /&gt;
&lt;br /&gt;
Let $\sigma(f)$ be the other fixpoint of $f$ (besides 0).&lt;br /&gt;
&lt;br /&gt;
...&lt;br /&gt;
&lt;br /&gt;
$$\sigma(f) = 2\pi i \alpha(f)(1+o(1)), \quad\text{as}\quad f\to f_0$$&lt;br /&gt;
&lt;br /&gt;
=== Comments ===&lt;br /&gt;
&lt;br /&gt;
By the comment before, we can say that $\sigma(f)$ lies roughly in the sector of angle $(\frac{\pi}{4},\frac{3\pi}{4})$ above the tip 0.&lt;br /&gt;
&lt;br /&gt;
== Proposition 3.2.2 ==&lt;br /&gt;
Let $f_0\in\mathcal{F}_0$. There exists a neighborhood $\mathcal{N}_0$ of $f_0$ (in the sense of the topology defined in 2.5.1) such that if $f\in\mathcal{N}_0\cap \mathcal{F}_1$, then there exist closed Jordan domains $S_{-,f}$, $S_{+,f}$ and analytic functions $\Phi_{-,f}$, $\Phi_{+,f}$ satisfying the following:&lt;br /&gt;
&lt;br /&gt;
(i) $S_{+,f}$ is bounded by an arc $\ell_{\pm}$ and its image $f(\ell_{\pm})$ such that $\ell_{\pm}$ joins two fixed points $\{0,\sigma(f)\}$, $\ell_{\pm}\cap f(\ell_{\pm}) = \{0,\sigma(f)\}$ and $S_{-,f}\cap S_{+,f} = \{0,\sigma(f)\}$; &lt;br /&gt;
&lt;br /&gt;
(ii) $\Phi_{\pm,f}$ is defined, analytic and injective in a neighborhood of $S&amp;#039;_{\pm,f} = S_{\pm,f}\setminus \{0,\sigma(f)\}$;&lt;br /&gt;
&lt;br /&gt;
(iii) if $z\in S&amp;#039;_{-,f}$ then there is an $n\ge 1$ such that $f^n(z)\in S&amp;#039;_{+,f}$ and for the smallest such $n$,&lt;br /&gt;
\[ \Phi_{+,f}(f^n(z)) = \Phi_{-,f}(z) - \frac{1}{\alpha(f)} + n \]&lt;br /&gt;
&lt;br /&gt;
(iv) when $f\in\mathcal{F}_1$ tends to $f_0$, $S_{\pm,f}\to S_{\pm,0}\cup \{0\}$ in the Hausdorff metric, and $\Phi_{\pm,f}\to \Phi_{\pm,0}$ in the topology defined in 2.5.1.&lt;br /&gt;
&lt;br /&gt;
== Proposition 4.4.1 ==&lt;br /&gt;
&amp;amp;#91;p. 356&amp;amp;#93;&lt;br /&gt;
&lt;br /&gt;
Let $f_0\in\mathcal{F}_0$, there exists a neighborhood $\mathcal{N}_0$ of $f_0$ (in the previously described &amp;quot;compact-open topology with domain of definition&amp;quot;), such that if $f\in \mathcal{N}_0 \cap \mathcal{F}_1$, then there exist large $\xi_0, \eta_0&amp;gt;0$, and analytic maps $\ph_f\colon D(\ph_f)\to\overline{\C}$ and $\tilde{\mathcal{R}}_f\colon D(\tilde{\mathcal{R}}_f)\to \C$ satisfying the following:&lt;br /&gt;
# $D(\ph_f)$ contains the set $$ \mathcal{Q}_f = \{ w\in\C\colon |\arg(-w-\xi_0)| &amp;lt; \frac{2\pi}{3}, |\arg(w+\frac{1}{\alpha(f)}-\xi_0)|&amp;lt;\frac{2\pi}{3} \} $$ and $\ph_f(D(\ph_f)) \subseteq D(f)$; If $w, w+1\in D(\ph_f)$ then $$ \ph_f(w+1)=f(\ph_f(w)) $$ $\ph_f(w)\to 0$ when $w\in \mathcal{Q}_f$ and $\Im(w)\to\infty$; $\ph_f(w)\to\sigma(f)$ when $w\in\mathcal{Q}_f$ and $\Im(w)\to -\infty$.&lt;br /&gt;
# $D(\tilde{\mathcal{R}}_f)$ contains $\{ w\in\C\colon |\Im(w)| &amp;gt; \eta_0\}$ and is invariant under $T(w)=w+1$; if $w\in D(\tilde{\mathcal{R}}_f)$ then $$\tilde{\mathcal{R}}_f(w+1)=\tilde{\mathcal{R}}(w)+1;$$ $\tilde{\mathcal{R}}_f(w)-w$ tends to $-\frac{1}{\alpha(f)}$ when $\Im(w)\to\infty$; to a constant when $\Im(w)\to -\infty$.&lt;br /&gt;
# If $w\in D(\tilde{\mathcal{R}}_f)\cap D(\ph_f)$ and $w&amp;#039;=\tilde{\mathcal{R}}_f(w)+n\in D(\ph_f)$ for some $n\in\Z$ then $$f^n(\ph_f(w))=\ph_f(w&amp;#039;)\quad \text{for}\quad n\ge 0, \quad f^{-n}(\ph_f(w&amp;#039;))=\ph_f(w)\quad \text{for}\quad n&amp;lt;0$$ Moreover if $|\arg(w&amp;#039;+\frac{1}{2\alpha(f)}-\xi_0)|&amp;lt;\frac{2\pi}{3}$ then $n&amp;gt;0$.&lt;br /&gt;
# When $f\in\mathcal{F_1}$ and $f\to f_0$ $$\ph_f\to\ph_0\quad\text{and}\quad \tilde{\mathcal{R}}_f + \frac{1}{\alpha(f)} \to \tilde{\mathcal{E}}_{f_0}$$&lt;br /&gt;
&lt;br /&gt;
&amp;lt;references/&amp;gt;&lt;/div&gt;</summary>
		<author><name>Bo198214</name></author>
	</entry>
	<entry>
		<id>https://tetrationforum.org/hyperops_wiki/index.php?title=Shishikura_perturbed_Fatou_coordinates&amp;diff=147</id>
		<title>Shishikura perturbed Fatou coordinates</title>
		<link rel="alternate" type="text/html" href="https://tetrationforum.org/hyperops_wiki/index.php?title=Shishikura_perturbed_Fatou_coordinates&amp;diff=147"/>
		<updated>2013-02-19T21:32:18Z</updated>

		<summary type="html">&lt;p&gt;Bo198214: added new section from Shishikura&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Shishikura writes&amp;lt;ref name=&amp;quot;Shishikura2000&amp;quot;&amp;gt;Shishikura, M. (2000). Bifurcation of parabolic fixed points. In Lei, Tan, The Mandelbrot set, theme and variations. Cambridge: Cambridge University Press. Lond. Math. Soc. Lect. Note Ser. 274, 325-363 (2000)&amp;lt;/ref&amp;gt; the following&lt;br /&gt;
&lt;br /&gt;
== $\mathcal{F}_0$ ==&lt;br /&gt;
&amp;amp;#91;p. 327&amp;amp;#93;&lt;br /&gt;
 &lt;br /&gt;
If $f_0&amp;#039;&amp;#039;(0)\neq 0$ by another coordinate change we may assume that $f_0&amp;#039;&amp;#039;(0)=1$, so define&lt;br /&gt;
$$ \mathcal{F}_0 = \{ f_0 \colon f_0 \quad\text{is defined and analytic in a neighborhood of 0}\quad f_0(0)=0, f_0&amp;#039;(0)=1, f_0&amp;#039;&amp;#039;(0)=1\}$$&lt;br /&gt;
&lt;br /&gt;
== Neighborhood of $f$ in the compact-open topology with domain of definition ==&lt;br /&gt;
&amp;amp;#91; p. 332 &amp;amp;#93;&lt;br /&gt;
&lt;br /&gt;
In what follows a map $f$ is always associated with its domain of definition $D(f)$. That is two maps are considered as distinct if they have distinct domains, even if the one is an extension of the other. A neighborhood of an analytic map $f\colon D(f)\to\overline{\C}$ is a set containing&lt;br /&gt;
$$\{ g \colon g \quad\text{is analytic},\quad D(g)\supset K, \sup_{z\in K} d(f(z)-g(z))&amp;lt;\eps \} $$&lt;br /&gt;
where $K$ is a compact set in $D(f)$, $\eps&amp;gt;0$ and $d(.,.)$ is the spherical metric.&lt;br /&gt;
A sequence $(f_n)$ converges to $f$ in this topology if and only if for any compact set $K\subset D(f)$ there exists $n_0$ such that $K\subset D(f_n)$ for all $n\ge n_0$ and $f_n|_K\to f|_K$ uniformly on $K$ as $n\to\infty$. The system of these neighborhoods define the &amp;quot;compact-open topology together with the domain of defintion&amp;quot;, which is unfortunately not Hausdorff, since an extension of $f$ is contained in any neighborhood of $f$.&lt;br /&gt;
&lt;br /&gt;
For $b_1,b_2\in\C$ with $\Re(b_1)&amp;lt;\Re(b_2)$ define &lt;br /&gt;
$$Q(b_1,b_2)=\{z\in\C\colon \Re(z-b_1)&amp;gt;-|\Im(z-b_1)|, \Re(z-b_2)&amp;gt;|\Im(z-b_2)|\}$$&lt;br /&gt;
If $b_1=-\infty$ (resp. $b_2=\infty$) then the corresponding condition should be removed.&lt;br /&gt;
&lt;br /&gt;
== Proposition 2.5.2 ==&lt;br /&gt;
&amp;amp;#91;p. 333&amp;amp;#93;&lt;br /&gt;
&lt;br /&gt;
Let $f$ be a holomorphic function defined on $Q=Q(b_1,b_2)$ with $\Re(b_2)&amp;gt;\Re(b_1)+2$ (here $b_1$ or $b_2$ may be $-\infty$ or $\infty$). Suppose &lt;br /&gt;
$$|F(z)-(z+1)|&amp;lt;\frac{1}{4},\quad |F&amp;#039;(z)-(z+1)|&amp;lt;\frac{1}{4}\quad \text{for all}\quad z\in Q.$$&lt;br /&gt;
&lt;br /&gt;
Then&lt;br /&gt;
# $F$ is univalent &amp;amp;#91;means injective&amp;amp;#93; on $Q$.&lt;br /&gt;
# Let $z_0\in Q$ be a point such that $\Re(b_1)&amp;lt;\Re(z_0)&amp;lt;\Re(b_2)-\frac{5}{4}$. Denote by $S$ the closed region (a strip) bounded by the two curves $\ell=\{z_0+i y\colon y\in\R\}$ and $F(\ell)$. Then for any $z\in Q$ there exist a unique $n\in \Z$ such that $F^n(z)$ is defined and belongs to $S-F(\ell)$.&lt;br /&gt;
# There exists an univalent function $\Phi\colon Q\to \C$ satisfying $$\Phi(F(z))=\Phi(z)+1$$ whenever both sides are defined. Moreover $\Phi$ is unique up to an addition of a constant.&lt;br /&gt;
# Fix a point $z_0\in Q$. If we normalize $\Phi$ by $\Phi(z_0)=0$ then the correspondence $F\mapsto \Phi$ is continuous with respect to the compact-open topology.&lt;br /&gt;
&lt;br /&gt;
== $\mathcal{F}$, $\mathcal{F}_1$ and $\alpha(f)$ ==&lt;br /&gt;
&amp;amp;#91;p. 339&amp;amp;#93;&lt;br /&gt;
&lt;br /&gt;
$$ \mathcal{F} = \{ f \colon f \quad\text{is defined and analytic in a neighborhood of 0}\quad f(0)=0, f_0&amp;#039;(0)\neq 0\}$$&lt;br /&gt;
For $f\in \mathcal{F}$ we express the derivative &lt;br /&gt;
$$f&amp;#039;(0)=\exp(2\pi i \alpha(f))$$&lt;br /&gt;
where $\alpha(f)\in\C$ and $-\frac{1}{2} &amp;lt; \Re(\alpha(f)) \le \frac{1}{2}$ our study is focussed on the maps in the following class&lt;br /&gt;
$$ \mathcal{F}_1 = \{ f\in \mathcal{F}\colon |\arg(\alpha(f))| &amp;lt; \frac{\pi}{4}\} $$&lt;br /&gt;
&lt;br /&gt;
=== Comments ===&lt;br /&gt;
&lt;br /&gt;
By the definition we have $$&lt;br /&gt;
\begin{align*}&lt;br /&gt;
\log(f&amp;#039;(0))&amp;amp;=2\pi i\alpha(f)=2\pi i re^{i\beta}=2\pi r e^{i(\beta+\frac{\pi}{2})}\\&lt;br /&gt;
\arg(\log(f&amp;#039;(0))&amp;amp;=\beta+\frac{\pi}{2}&lt;br /&gt;
\end{align*}$$&lt;br /&gt;
so the condition for $\mathcal{F}_1$ is&lt;br /&gt;
$|\arg(\log(f&amp;#039;(0)))-\frac{\pi}{2}|&amp;lt;\frac{\pi}{4}$ or&lt;br /&gt;
$$\frac{\pi}{4} &amp;lt; \arg(\log(f&amp;#039;(0)) &amp;lt; \frac{3\pi}{4}$$&lt;br /&gt;
&lt;br /&gt;
== $\sigma(f)$ ==&lt;br /&gt;
&amp;amp;#91;p. 340&amp;amp;#93;&lt;br /&gt;
&lt;br /&gt;
Let $\sigma(f)$ be the other fixpoint of $f$ (besides 0).&lt;br /&gt;
&lt;br /&gt;
...&lt;br /&gt;
&lt;br /&gt;
$$\sigma(f) = 2\pi i \alpha(f)(1+o(1)), \quad\text{as}\quad f\to f_0$$&lt;br /&gt;
&lt;br /&gt;
=== Comments ===&lt;br /&gt;
&lt;br /&gt;
By the comment before, we can say that $\sigma(f)$ lies roughly in the sector of angle $(\frac{\pi}{4},\frac{3\pi}{4})$ above the tip 0.&lt;br /&gt;
&lt;br /&gt;
== Proposition 3.2.2 ==&lt;br /&gt;
Let $f_0\in\mathcal{F}_0$. There exists a neighborhood $\mathcal{N}$ of $f_0$ (in the sense of the topology defined in 2.5.1) such that if $f\in\mathcal{N}_0\cap \mathcal{F}_1, then there exist closed Jordan domains $S_{-,f}$, $S_{+,f}$ and analytic functions $\Phi_{-,f}$, $\Phi_{+,f}$ satisfying the following:&lt;br /&gt;
&lt;br /&gt;
(i) $S_{+,f}$ is bounded by an arc $\ell_{\pm}$ and its image $f(\ell_{\pm})$ such that $\ell_{\pm}$ joins two fixed points $\{0,\sigma(f)\}$, $\ell_{\pm}\cap f(\ell_{\pm}) = \{0,\sigma(f)\}$ and $S_{-,f}\cap S_{+,f} = \{0,\sigma(f)\}$; &lt;br /&gt;
&lt;br /&gt;
(ii) $\Phi_{\pm,f}$ is defined, analytic and injective in a neighborhood of $S&amp;#039;_{\pm,f} = S_{\pm,f}\setminus \{0,\sigma(f)\}$;&lt;br /&gt;
&lt;br /&gt;
(iii) if $z\in S&amp;#039;_{-,f}$ then there is an $n\ge 1$ such that $f^n(z)\in S&amp;#039;_{+,f}$ and for the smallest such $n$,&lt;br /&gt;
\[ \Phi_{+,f}(f^n(z)) = \Phi_{-,f}(z) - \frac{1}{\alpha(f)} + n \]&lt;br /&gt;
&lt;br /&gt;
(iv) when $f\in\mathcal{F}_1$ tends to $f_0$, $S_{\pm,f}\to S_{\pm,0}\cup \{0\}$ in the Hausdorff metric, and $\Phi_{\pm,f}\to \Phi_{\pm,0}$ in the topology defined in 2.5.1.&lt;br /&gt;
&lt;br /&gt;
== Proposition 4.4.1 ==&lt;br /&gt;
&amp;amp;#91;p. 356&amp;amp;#93;&lt;br /&gt;
&lt;br /&gt;
Let $f_0\in\mathcal{F}_0$, there exists a neighborhood $\mathcal{N}_0$ of $f_0$ (in the previously described &amp;quot;compact-open topology with domain of definition&amp;quot;), such that if $f\in \mathcal{N}_0 \cap \mathcal{F}_1$, then there exist large $\xi_0, \eta_0&amp;gt;0$, and analytic maps $\ph_f\colon D(\ph_f)\to\overline{\C}$ and $\tilde{\mathcal{R}}_f\colon D(\tilde{\mathcal{R}}_f)\to \C$ satisfying the following:&lt;br /&gt;
# $D(\ph_f)$ contains the set $$ \mathcal{Q}_f = \{ w\in\C\colon |\arg(-w-\xi_0)| &amp;lt; \frac{2\pi}{3}, |\arg(w+\frac{1}{\alpha(f)}-\xi_0)|&amp;lt;\frac{2\pi}{3} \} $$ and $\ph_f(D(\ph_f)) \subseteq D(f)$; If $w, w+1\in D(\ph_f)$ then $$ \ph_f(w+1)=f(\ph_f(w)) $$ $\ph_f(w)\to 0$ when $w\in \mathcal{Q}_f$ and $\Im(w)\to\infty$; $\ph_f(w)\to\sigma(f)$ when $w\in\mathcal{Q}_f$ and $\Im(w)\to -\infty$.&lt;br /&gt;
# $D(\tilde{\mathcal{R}}_f)$ contains $\{ w\in\C\colon |\Im(w)| &amp;gt; \eta_0\}$ and is invariant under $T(w)=w+1$; if $w\in D(\tilde{\mathcal{R}}_f)$ then $$\tilde{\mathcal{R}}_f(w+1)=\tilde{\mathcal{R}}(w)+1;$$ $\tilde{\mathcal{R}}_f(w)-w$ tends to $-\frac{1}{\alpha(f)}$ when $\Im(w)\to\infty$; to a constant when $\Im(w)\to -\infty$.&lt;br /&gt;
# If $w\in D(\tilde{\mathcal{R}}_f)\cap D(\ph_f)$ and $w&amp;#039;=\tilde{\mathcal{R}}_f(w)+n\in D(\ph_f)$ for some $n\in\Z$ then $$f^n(\ph_f(w))=\ph_f(w&amp;#039;)\quad \text{for}\quad n\ge 0, \quad f^{-n}(\ph_f(w&amp;#039;))=\ph_f(w)\quad \text{for}\quad n&amp;lt;0$$ Moreover if $|\arg(w&amp;#039;+\frac{1}{2\alpha(f)}-\xi_0)|&amp;lt;\frac{2\pi}{3}$ then $n&amp;gt;0$.&lt;br /&gt;
# When $f\in\mathcal{F_1}$ and $f\to f_0$ $$\ph_f\to\ph_0\quad\text{and}\quad \tilde{\mathcal{R}}_f + \frac{1}{\alpha(f)} \to \tilde{\mathcal{E}}_{f_0}$$&lt;br /&gt;
&lt;br /&gt;
&amp;lt;references/&amp;gt;&lt;/div&gt;</summary>
		<author><name>Bo198214</name></author>
	</entry>
	<entry>
		<id>https://tetrationforum.org/hyperops_wiki/index.php?title=Hyperbolic_fixpoint&amp;diff=134</id>
		<title>Hyperbolic fixpoint</title>
		<link rel="alternate" type="text/html" href="https://tetrationforum.org/hyperops_wiki/index.php?title=Hyperbolic_fixpoint&amp;diff=134"/>
		<updated>2011-06-09T18:11:11Z</updated>

		<summary type="html">&lt;p&gt;Bo198214: forgot some terms&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;A hyperbolic fixpoint is a [[fixpoint]] $a$ of $f$ such that $|f&amp;#039;(a)|\neq 0,1$.&lt;br /&gt;
&lt;br /&gt;
For a locally analytic function with hyperbolic fixpoint at $0$, i.e. $f(z)=c_1 z + c_2z^2 + \dots$, $|c_1|\neq 0,1$, there is always a locally analytic and injective function $\sigma$ that satisfies the [[Schröder equation]]&lt;br /&gt;
$$\sigma(f(z))=c_1 \sigma(z))$$&lt;br /&gt;
$\sigma$ is unique up to a multiplicative constant and is called the [[Schröder coordinates]] of $f$ at 0.&lt;/div&gt;</summary>
		<author><name>Bo198214</name></author>
	</entry>
	<entry>
		<id>https://tetrationforum.org/hyperops_wiki/index.php?title=Schr%C3%B6der_iterate&amp;diff=133</id>
		<title>Schröder iterate</title>
		<link rel="alternate" type="text/html" href="https://tetrationforum.org/hyperops_wiki/index.php?title=Schr%C3%B6der_iterate&amp;diff=133"/>
		<updated>2011-06-08T08:39:23Z</updated>

		<summary type="html">&lt;p&gt;Bo198214: changed to coordinate&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;A way to compute regular iterates of a function $f$ with [[attracting fixpoint|attracting]] or [[hyperbolic fixpoint]] $a$.&lt;br /&gt;
&lt;br /&gt;
For $z$ in the immediate basin of attraction of the attracting fixpoint $a$ and $f&amp;#039;(a)=c_1$, it is:&lt;br /&gt;
$$f^t(z)=\lim_{n\to\infty} f^{-n}(c_1^t f^n(z))$$&lt;br /&gt;
&lt;br /&gt;
Or $\sigma$ being the [[Schröder coordinate]] of $f$ at $a$, we have:&lt;br /&gt;
$$f^t(z)=\sigma^{-1}(c_1^t \sigma(z))$$&lt;/div&gt;</summary>
		<author><name>Bo198214</name></author>
	</entry>
	<entry>
		<id>https://tetrationforum.org/hyperops_wiki/index.php?title=B%C3%B6ttcher_iterate&amp;diff=132</id>
		<title>Böttcher iterate</title>
		<link rel="alternate" type="text/html" href="https://tetrationforum.org/hyperops_wiki/index.php?title=B%C3%B6ttcher_iterate&amp;diff=132"/>
		<updated>2011-06-08T08:38:22Z</updated>

		<summary type="html">&lt;p&gt;Bo198214: first draft&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;A way to compute the regular iterates of a function $f$ with [[super-attracting fixpoint]] $a$.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For $f(z)=c_m (z-a)^m + c_{m+1} (z-a)^{m+1} + \dots$ the Böttcher iterate is:&lt;br /&gt;
$$f^t(z)=\lim_{n\to\infty} f^{-n}(f^n(z)^{m^t})$$&lt;br /&gt;
&lt;br /&gt;
Or if $\beta$ is the [[Böttcher coordinate]] of $f$ at $a$, then &lt;br /&gt;
$$f^t(z)=\beta^{-1}\left(\beta(z)^{m^t}\right)$$&lt;/div&gt;</summary>
		<author><name>Bo198214</name></author>
	</entry>
</feed>